►Nboost | |
►Nnumeric | |
►Nbindings | |
►Ndetail | |
Cadaptor< Eigen::Map< Matrix >, Id, Enable > | Specialize numeric bindings traits for Eigen::Map |
Cadaptor< Eigen::Matrix< T, Rows, 1, Options >, Id, Enable > | |
Cadaptor< mpqc::matrix< T, Options >, Id, Enable > | Specialize numeric bindings traits for mpqc::matrix |
►Nproperty_tree | |
Ctranslator_between< std::basic_string< Ch, Traits, Alloc >, sc::XMLDataStream< T, val > > | |
►Ndetail | |
Cbasis_iterable | |
►Nmpqc | Contains new MPQC code since version 3 |
►Nci | |
►CCI | CI class template |
CIO | |
CSort | Compare-by-rank functor |
CConfig | CI configuration |
CExcitation | One-particle excitation from string I to string J, {sign, ij, I, J} |
CExcitations | Vector of single particle excitations from I to J subspace |
CFull | |
CRestricted | Restricted CI Functor |
CSpace | A CI space, marked by Spin S and rank |
CSpin | Electron spin |
►CString | |
CIndex | Implements a dense String->index map, appropriate for a full CI string sets |
CList | String::List represents a set of String objects |
Corbitals | |
CSubspace | A range of a space where all objects in the subspace range are assumed to have the same space rank |
CSubspace< Any > | A subspace specialization that "discard" the spin parameter |
►CSubspaceBlock | |
CSort | |
CSubspaceGrid | Grid of subspaces, represented as blocks of determinants defined by alpha/beta pair, along with sparsity information |
►CVector | Block CI Vector, with 1-d (vector) and 2-d (matrix) access |
CBlock1d | 1-d vector sub-block |
CBlock2d | 2-d vector sub-block |
►Ndetail | |
►NArrayServer | |
►Carray_proxy | |
CDescriptor | |
CSegment | |
CMessage | |
CThread | |
►NFile | Implementation details |
CAttribute | |
CObject | A reference-counted HDF5 handle object, superclass for eg File, Dataset, Attribute, etc |
CProperties | |
Cstatic_container | |
Cthreadsafe | HDF5 may not be threadsafe, in that case mpqc::mutex::global is used |
►NTensor | |
Cassign | |
Cdivide_assign | |
Cintegral_tie | Index tie wrapper |
Cis_integral | |
Cis_integral_tuple | "returns" true if every element of tuple T is an integral type |
Cminus_assign | |
Cmultiply_assign | |
Cplus_assign | |
Crange_tie | Range tie wrapper |
Carray_core_driver | |
Carray_file_driver | |
Carray_impl | |
Carray_impl< T, array_core_driver > | |
Carray_impl< T, array_file_driver > | |
Carray_parallel_impl | |
Carray_thread_comm | |
Carray_tile | |
CArrayBase | |
CArraySocket | |
CArrayTile | |
►Nlcao | |
CIntegrals | Wraps an MPQC integral engine (e.g |
CShell | |
►NMPI | |
►CComm | MPI_Comm object wrapper/stub |
COStream | |
CTask | Distributed task |
►Nomp | |
Cmutex | |
Ctask | |
►Npurification | |
Cperformance | |
►NTA | |
►Ncluster | |
CClusterAtom | |
CClDFGEngine | |
CCLHF | |
CCLSCF | The taclscf class is the base class for implementing self-consistent proceedure for closed-shell molecules in MPQC3 |
CGEngineBase | |
CIntegralEnginePool | IntegralEnginePool is a class that will take a Ref<Engine> as a prototype and then clone it multiple times such that each thread has its own integral engine |
CKCluster | Class holds the information about the differnt clusters in k-means tiling |
CSCF | |
CShellOrder | Determines the clustering of shells based on k-means clustering |
CTiledBasisSet | TiledBasisSet is a GaussianBasisSet in which basis functions/shells are grouped into tiles ("blocks") |
CWavefunction | Wavefunction represents an electronic wave function expressed in terms of a basis set of atomic orbitals |
CArray | Array implementation |
Ccstring | Cstring-like object to cast a value to const char*< > string |
CException | MPQC exception class |
►CFile | Top-level file object that holds groups |
CDataset | Array-like collection of data |
CDataspace | A subset of File::Dataset |
CDriver | Base file driver |
CGroup | Directory-like container that holds datasets and other groups |
CPOSIXDriver | POSIX I/O file driver, the default |
CMADNESSRuntime | |
►Cmatrix | Matrix class derived from Eigen::Matrix with additional MPQC integration |
CAssignable | An interface to enable matrix assignment from other containers |
►Cmutex | Static mutex instances |
Cglobal_mutex_tag | |
►Crange | |
Cblock_list | |
Ctie | Boost::tuple tie wrapper |
CRange | |
Cstatic_mutex | Static mutex factory |
CTensor | Tensor reference class |
CTensorBase | Tensor base class |
►CTensorColumnMajor | Tensor column major (i.e. first dimension is contiguous) storage order |
Cmake_index | |
CTensorDimensionsException | |
CTensorIndexException | |
CTensorRangeException | |
CTensorRef | Tensor reference class |
►CTensorRowMajor | Tensor row major (i.e. last dimension is contiguous) storage order |
Cmake_index | |
Ctimer | |
Cvector | Vector class derived from Eigen::Matrix with additional MPQC integration |
CWorld | World is a wrapper around madness::World |
►Nsc | Contains all MPQC code up to version 3 |
►Ncadf | |
►Nassignments | |
CAssignments | |
CAtomCluster | |
►Ndetail | |
Cbegin_index_less | |
Cderef_compare | |
Cderef_compare< boost::shared_ptr< T >, compare > | |
Cderef_compare< T *, compare > | |
Cindex_less | |
Cmore_work | |
CAssignableAtom | |
CAssignableItem | |
CAssignableShell | |
CAssignableShellPair | |
CAssignmentBin | |
CAssignmentBinRow | |
CAssignmentGrid | |
CHistogram2d | |
CNode | |
CProductBlock | |
CTreeBlock | |
CTreeMatrix | |
►Ndetail | |
C__to_extern_C_eval | |
C_CABS_singles_h0t1 | This functor helps to implement conjugate gradient CABS singles solver |
C_Merger | |
C_OrbResponse | This functor helps to implement orbital response |
CContainerAdaptor | |
CContainerAdaptor< RefDiagSCMatrix > | |
CDDPhiEvalCreator | |
CDeltaFunctionEvalCreator | |
CDeltaFunctionEvalCreator< 2 > | |
CDeltaFunctionEvalCreator< 3 > | |
CDeltaFunctionEvalCreator< 4 > | |
Cdiag_precond2 | Makes a diagonal 2-index preconditioner: pc_x^y = -1/ ( <x|O1|x> - <y|O2|y> ) |
Cdiag_precond4 | Makes a diagonal 4-index preconditioner: pc_xy^zw = -1/ ( <x|O1|x> + <y|O2|y> - <z|O3|z> - <w|O4|w> ) |
CDPhiEvalCreator | |
Ce_ij | |
CEqualTypes | |
CEqualTypes< A, A > | |
CERIEvalCreator | |
CERIEvalCreator< 2 > | |
CERIEvalCreator< 3 > | |
CERIEvalCreator< 4 > | |
CFockMatrixType | |
►CFockMatrixType< false > | |
CFactory | |
►CFockMatrixType< true > | |
CFactory | |
CG12DKHEvalCreator | |
CG12DKHEvalCreator< 2 > | |
CG12DKHEvalCreator< 3 > | |
CG12DKHEvalCreator< 4 > | |
CG12EvalCreator | |
CG12EvalCreator< 2 > | |
CG12EvalCreator< 3 > | |
CG12EvalCreator< 4 > | |
CG12NCEvalCreator | |
CG12NCEvalCreator< 2 > | |
CG12NCEvalCreator< 3 > | |
CG12NCEvalCreator< 4 > | |
CG12T1G12EvalCreator | |
CG12T1G12EvalCreator< 2 > | |
CG12T1G12EvalCreator< 3 > | |
CG12T1G12EvalCreator< 4 > | |
CGetValue | GetValue(keyval, key, i) grabs the value corresponding to key |
CGetValue< bool > | |
CGetValue< char > | |
CGetValue< double > | |
CGetValue< float > | |
CGetValue< int > | |
CGetValue< long > | |
CGetValue< std::size_t > | |
CGetValue< std::string > | |
Chash_ | |
Chash_< ShellIndexWithValue > | |
CHCoreEvalCreator | |
Cindex_equal_ | |
CMakeTwoBodyTransform | |
CMakeTwoBodyTransform< false > | |
CMakeTwoBodyTransform< true > | |
CMuEvalCreator | |
CNeedDF | |
CNeedDF< TwoBodyMOIntsTransform_ixjy_df > | |
CNonsingletonCreationPolicy | NonsingletonCreationPolicy is used to create non-Singletons on heap |
COneBodyEvalCreator | |
COrbital_relaxation_Abjai | |
CP4EvalCreator | |
CParsedTwoBodyIntKey | |
CParsedTwoBodyIntKey< 2 > | |
CParsedTwoBodyIntKey< 3 > | |
CParsedTwoBodyIntKey< 4 > | |
CPhiEvalCreator | |
Cpoint | |
CQEvalCreator | |
CR120G12EvalCreator | |
CR120G12EvalCreator< 2 > | |
CR120G12EvalCreator< 3 > | |
CR120G12EvalCreator< 4 > | |
CR12EvalCreator | |
CR12EvalCreator< 2 > | |
CR12EvalCreator< 3 > | |
CR12EvalCreator< 4 > | |
CR12m1G12EvalCreator | |
CR12m1G12EvalCreator< 2 > | |
CR12m1G12EvalCreator< 3 > | |
CR12m1G12EvalCreator< 4 > | |
Cselfenergy_denom | Makes a pseudo-3-index (4-index, but first index is dummy) self-energy denominator: (se_den)_{xyz} = 1/ ( E + <x|Y|x> - <y|X1|y> - <z|X2|z>); |
CSEvalCreator | |
CSEvalCreator< 2u > | |
CSingletonCreationPolicy | SingletonCreationPolicy is used to create Singletons |
CSumMerger | |
CTEvalCreator | |
CToDensityFittingType | |
CToDensityFittingType< TwoBodyMOIntsTransform_ikjy > | |
CToDensityFittingType< TwoBodyMOIntsTransform_iRjS > | |
CToDensityFittingType< TwoBodyMOIntsTransform_ixjy > | |
CTriangleWriter | |
CTriangleWriter< Derived, Eigen::Lower > | |
Ctuple | |
CTwoBodyEvalCreator | |
CTwoBodyEvalCreator< NumCenters, TwoBodyOperSet::DeltaFunction > | |
CTwoBodyEvalCreator< NumCenters, TwoBodyOperSet::ERI > | |
CTwoBodyEvalCreator< NumCenters, TwoBodyOperSet::G12 > | |
CTwoBodyEvalCreator< NumCenters, TwoBodyOperSet::G12_T1_G12 > | |
CTwoBodyEvalCreator< NumCenters, TwoBodyOperSet::G12DKH > | |
CTwoBodyEvalCreator< NumCenters, TwoBodyOperSet::G12NC > | |
CTwoBodyEvalCreator< NumCenters, TwoBodyOperSet::R12 > | |
CTwoBodyEvalCreator< NumCenters, TwoBodyOperSet::R12_0_G12 > | |
CTwoBodyEvalCreator< NumCenters, TwoBodyOperSet::R12_m1_G12 > | |
CTwoBodyIntEval | |
CTwoBodyIntEval< 2 > | |
CTwoBodyIntEval< 3 > | |
CTwoBodyIntEval< 4 > | |
CTwoBodyMOIntsRuntimeParams | |
CTwoBodyMOIntsRuntimeParams< 2 > | |
CTwoBodyMOIntsRuntimeParams< 3 > | |
CTwoBodyMOIntsRuntimeParams< 4 > | 4-center 2-body integrals can use density fitting |
Cvertex | |
Cvertices | |
CVEvalCreator | |
►Nexpressions | |
Cdiag_tensor2_op | |
CTGeminalGenerator | Makes a geminal T tensor |
Ctrace_tensor2_op | |
►Nfastpairiter | |
CMOPairIter | SpinMOPairIter iterates over pairs of spinorbitals of spin case Spin12 This class differs from other MOPairIter classes: 1) cannot start from arbitrary IJ, only IJ=0; 2) error checking maximally reduced |
►Nlibint2 | |
CInt2eCreator | |
►NManyBodyTensors | Contains classes used to compute many-body tensors |
CApply_H0minusE0 | Applies (H0 - E0) |
CApply_Identity | Tensor elements are <pq||rs> |
CApply_Inverse_H0minusE0 | Applies (H0 - E0)^{-1}, e.g. MP2 T2 tensor elements are <ij||ab> /(e_i + e_j - e_a - e_b) |
CApply_Inverse_Sqrt_H0minusE0 | Applies 1.0/sqrt(H0-E0) MP2 pseudo-T2 (S2) tensor elements are <ij||ab> /sqrt(|e_i + e_j - e_a - e_b|) such that MP2 pair energies are the diagonal elements of S2 * S2.t() |
►Nmath | |
CGaussian1D | Gaussian1D(k,x) = c x^k exp(-a*x^2) |
CPowerExponential1D | PowerExponential1D(k,l,x) = c x^k exp(-a*x^l) |
CSlater1D | Slater1D(k,x) = |
►Nmbptr12 | |
CABS_OBS_Contraction | ABS_OBS_Contraction contracts 2 square nobs-by-nobs blocks for the ABS approach |
CCABS_OBS_Contraction | CABS_OBS_Contraction contracts 2 square nobs-by-nobs blocks for the CABS approach |
CDirect_Contraction | Direct_Contraction is a straight scalar (dot) product of 2 rectangular blocks, scaled by scale |
CTwoParticleContraction | TwoParticleContraction contracts nrow-by-ncol bra- or ket-blocks of two 2-particle tensors i.e |
►Nmeta | |
Csplat_types | |
Csplat_values | |
►Nsma2 | |
CArray | Implements a block sparse tensor |
CArray24SCExtrapData | This permits an Array<2> and an Array<4> to be used with SelfConsistentExtrapolation derivatives |
CArray24SCExtrapError | This permits an Array<2> and an Array<4> to be used with SelfConsistentExtrapolation derivatives |
CArray2SCExtrapData | This permits Array<2>'s to be used with SelfConsistentExtrapolation derivatives |
CArray2SCExtrapError | This permits Array<2>'s to be used with SelfConsistentExtrapolation derivatives |
CArray4SCExtrapData | This permits Array<4>'s to be used with SelfConsistentExtrapolation derivatives |
CArray4SCExtrapError | This permits Array<4>'s to be used with SelfConsistentExtrapolation derivatives |
CArray6SCExtrapData | This permits Array<6>'s to be used with SelfConsistentExtrapolation derivatives |
CArray6SCExtrapError | This permits Array<6>'s to be used with SelfConsistentExtrapolation derivatives |
CBlockDistrib | Provides information about how blocks are distributed onto processes |
CBlockInfo | BlockInfo stores info about a block of data |
CBlockInfo< 0 > | |
CBlockInfo< 3 > | |
CBlockInfo< 4 > | |
CBlockIter | BlockIter loops through the all the indices within a block |
CBlockIter< 0 > | Blocksize == 0 specialization of BlockIter |
CCompleteBlockDistrib | Distribute blocks round-robin among processes using one or more index values |
CContractPart | Represents an array and symbolic indices in a contraction |
CContractProd | Represents a pairs of contracted array and their symbolic indices |
CContractUnion | |
CData | Data holds the values for each block |
CDivOperation | |
CIndex | An Index is used in the symbolic notation for contractions |
CIndexList | An IndexList is a vector of indices |
CIndexListLess | Functor for determining if one IndexList is less than another |
CIndicesLess | Functor for comparing a block's indices |
CIndicesLess< 0 > | Functor for comparing a block's indices |
CPairBlockDistrib | An implementation of BlockDistrib using PairMapping |
CPairMapping | Distributes pairs of indices among the processes |
CRange | An Range represent a set of integers, [0, N) |
CRepackScheme | Determine the cost of repacking arrays for a contraction |
CSumOperation | |
Ctriplet | Stores a triplet of data |
►Ntr1 | |
►Narray | |
Carray | Array idential to C++0X arrays |
Carray< T, 0 > | |
Cabs_greater | |
Cabs_less | Useful comparison functions |
CAccResult | This associates a result datum with an accuracy |
CAccResultInfo | This is like ResultInfo but the accuracy with which a result was computed as well as the desired accuracy are stored |
CAccumEffectiveH | |
CAccumH | AccumH computes additions to the one body Hamiltonian |
CAccumHNull | This specialization of AccumH does nothing |
CActiveMessage | Derivatives of ActiveMessage can be constructed in one process and executed in another by using ActiveMessageGrp |
CActiveMessageEcho | This is an ActiveMessage derivative used for testing |
CActiveMessageGrp | ActiveMessageGrp provides an implemention of active messages that sends objects derived from ActiveMessage to remote processes and causes their run member to be executed there |
CActiveMessageThread | This is a help class that is used by ActiveMessageGrp |
CActiveMsgMemoryGrp | The ActiveMsgMemoryGrp abstract class specializes the MsgMemoryGrp class |
CAggregateKeyVal | |
CALevelShift | |
CAlgorithmException | This exception is thrown whenever a problem with an algorithm is encountered |
CAM05Functional | Implements the Perdew-Burke-Ernzerhof (PBE) correlation functional |
CAngularIntegrator | An abstract base class for angular integrators |
CAnimatedObject | |
CAppearance | |
CApproximatePairWriter | |
CARMCIMemoryGrp | The ARMCIMemoryGrp concrete class provides an implementation of MsgMemoryGrp |
CAssertionFailed | This is thrown when an assertion fails |
CAssignedKeyVal | |
CAtom | Atom represents an atom in a Molecule |
CAtomicOrbitalSpace | This is an OrbitalSpace describing a set of atomic orbitals |
CAtomInfo | Information about atoms |
CAtomProximityColorizer | |
Cauto_time_accumulator | |
Cauto_vec | The auto_vec class functions much like auto_ptr, except it contains references to arrays |
►CAVLMap | |
Citerator | |
CAVLMapNode | |
►CAVLMMap | |
Cconst_iterator | |
Citerator | |
CAVLMMapNode | |
►CAVLSet | |
Citerator | |
CBacktrack | Implements backtrack line search algorithm |
Cbasis_element_iterator | |
Cbasis_element_with_value_iterator | |
CBasisElementData | |
CBasisElementIteratorDereference | |
CBasisFileSet | |
CBasisFunctionData | |
CBatchElectronDensity | This a more highly optimized than ElectronDensity since everything is precomputed |
CBcastState | This creates and forwards/retrieves data from either a BcastStateRecv or a BcastStateSend depending on the value of the argument to constructor |
CBcastStateInBin | BcastStateBin reads a file in written by StateInBin on node 0 and broadcasts it to all nodes so state can be simultaneously restored on all nodes |
CBcastStateRecv | BcastStateRecv does the receive part of a broadcast of an object to all nodes |
CBcastStateSend | BcastStateSend does the send part of a broadcast of an object to all nodes |
CBecke88XFunctional | Implements Becke's 1988 exchange functional |
CBeckeIntegrationWeight | Implements Becke's integration weight scheme |
CBEMSolvent | |
CBEMSolventH | This specialization of AccumH computes the contribution to the energy and one body Hamiltonian from a solvent using a polarizable continuum model |
CBendSimpleCo | Describes an bend internal coordinate of a molecule |
CBFGSUpdate | The DFPUpdate class is used to specify a Broyden, Fletcher, Goldfarb, and Shanno hessian update scheme |
CBiggestContribs | |
CBitArrayLTri | |
CBLevelShift | |
CBlockedDiagSCMatrix | Blocked DiagSCMatrix |
CBlockedSCElementOp | |
CBlockedSCElementOp2 | |
CBlockedSCElementOp3 | |
CBlockedSCMatrix | Blocked SCMatrix |
CBlockedSCMatrixKit | BlockedSCMatrixKit is a SCMatrixKit that produces blocked matrices |
CBlockedSCVector | |
CBlockedSymmSCMatrix | Blocked SymmSCMatrix |
CBoundsLibint2 | Computes log2 bounds for a particular Int2e evaluator |
CBuildIntV3 | |
►CCADFCLHF | A specialization of CLHF that uses concentric atomic density fitting to build fock matrices |
►CScreeningStatistics | |
CIteration | |
CCannotConstructMap | |
Ccanonical_aa | Can be used as a template argument to GenericPetiteList2 |
Ccanonical_aaaa | If the shell loop structure has 8 fold symmetry, then this should be used as the template argument to GenericPetiteList4 |
Ccanonical_aabb | If the shell loop structure has 2 fold symmetry between the first two indices and a 2 fold symmetry between the last two indices, then this should be used as the template argument to GenericPetiteList4 |
Ccanonical_aabc | If the shell loop structure has 2 fold symmetry between the first two indices, then this should be used as the template argument to GenericPetiteList4 |
Ccanonical_ab | Can be used as a template argument to GenericPetiteList2 |
Ccanonical_abab | If the shell loop structure has 2 fold symmetry between the bra and the ket then this should be used as the template argument to GenericPetiteList4 |
Ccanonical_abcc | If the shell loop structure has 2 fold symmetry between the last two indices, then this should be used as the template argument to GenericPetiteList4 |
Ccanonical_abcd | If the shell loop structure has no symmetry, then this should be used as the template argument to GenericPetiteList4 |
CCartesianBasisSet | CartesianBasisSet is obtained from the parent basis by converting spherical harmonic shells to cartesian counterparts |
CCartesianIter | CartesianIter gives the ordering of the Cartesian functions within a shell for the particular integrals specialization |
CCartesianIterCCA | |
CCartesianIterGAMESS | |
CCartesianIterV3 | |
CCartMolecularCoor | Implements Cartesian coordinates in a way suitable for use in geometry optimizations |
CCCR12 | CCR12 is the base class for CC and CC-R12 methods |
CCCR12_Info | CCR12_Info is the compilation of members that are used in CC and CC-R12 methods |
CCCR12_Triples | |
CCCSD | |
CCCSD_2Q_LEFT | |
CCCSD_2Q_RIGHT | |
CCCSD_2T_LEFT | |
CCCSD_2T_PR12_RIGHT | |
CCCSD_2T_R12_LEFT | |
CCCSD_2T_RIGHT | |
CCCSD_E | |
CCCSD_PT | |
CCCSD_PT_LEFT | |
CCCSD_PT_RIGHT | |
CCCSD_R12 | |
CCCSD_R12_E | |
CCCSD_R12_PT_RIGHT | |
CCCSD_R12_T1 | |
CCCSD_R12_T2 | |
CCCSD_Sub_Bar_R12 | |
CCCSD_Sub_Full_R12 | |
CCCSD_Sub_R12 | CCSD_Sub_R12 is the base class for some (2)R12 methods |
CCCSD_SUB_R12_LEFT | |
CCCSD_SUB_R12_RIGHT | |
CCCSD_T1 | |
CCCSD_T2 | |
CCCSDPR12 | |
CCCSDPR12_C | |
CCCSDPR12_T1 | |
CCCSDPR12_T2 | |
CCCSDT | |
CCCSDT_T1 | |
CCCSDT_T2 | |
CCCSDT_T3 | |
CCCSDTQ | |
CCCSDTQ_T2 | |
CCCSDTQ_T3 | |
CCCSDTQ_T4 | |
CCharacterTable | Workable character table for all of the non-cubic point groups |
Cchunk_allocator | |
CCI | CI is a configuration interaction ManyBodyWavefunction |
CClassDesc | This class is used to contain information about classes |
CCLHF | CLHF is a Hartree-Fock specialization of CLSCF |
CCLHFContribution | Computes components of the Fock matrix necessary for closed-shell calculations (i.e |
CCLKS | This provides a Kohn-Sham implementation for closed-shell systems |
CCLSCF | Base for classes implementing a self-consistent procedure for closed-shell molecules |
CColor | |
CCompute | Means of keeping results up to date |
CConcurrentCacheBase | |
CConcurrentCacheWithSymmetry | A cache of objects that can be safely accessed concurrently by threads that share memory |
CConcurrentCacheWithSymmetry< val_type, KeySymmetry< IdentityKeyPermutation< sizeof...(key_types)> >, key_types... > | Specialization for the identity |
CConcurrentCacheWithSymmetry< val_type, KeySymmetry< IdentityKeyPermutation< sizeof...(key_types)>, KeyTransposition< n_keys, idx1, idx2 > >, key_types... > | Specialization with only one transposition other than the identity |
CConjugateGradientSolver | Solves linear system a(x) = b using conjugate gradient solver where a is a linear function of x |
CConnollyShape | DiscreteConnollyShape and ConnollyShape should produce the same result |
CConsumableResources | ConsumableResources keeps track of consumable resources (memory, disk) |
CContiguousShellBlockList | |
Ccontribution | |
CConvergence | Used by the optimizer to determine when an optimization is converged |
►CCoreIntsEngine | CoreIntsEngine manages Boys, and other core integral, engines |
CEngine | |
CCorrelatedMOOrder | Order by occupation first, then by symmetry, then by energy |
CCorrelatedSpinMOOrder | Order by occupation first, then by spin, then by symmetry, then by energy |
CCorrelationTable | Correlation table between two point groups |
CCreateTransformHints | Provides hints to the constructors of a Transform class that help configure its implementation |
CCS2Sphere | |
CCSGrad34Qbtr | |
CCSGradErep12Qtr | |
CCSGradS2PDM | |
CCuspConsistentGeminalCoefficient | Computes fixed coefficients determined according to the cusp conditions for geminal (r12-dependent) functions that have been normalized so that coefficient of r12 in Taylor expansion around r12=0 is 1 |
CDA4_Tile | Tile of a 4-index tensor that's "evaluated" when needed by reading from DistArray4 |
CDA4_Tile34 | Tile of a <34> slice of <1234> that's "evaluated" when needed by reading from DistArray4 holding pqrs |
►CDebugger | Describes what should be done when a catastrophic error causes unexpected program termination |
CBacktrace | Creates a backtrace of a running program/thread |
CDecoratedOrbital | Orbital = index + attributes |
CDefaultPrintThresholds | Default print thresholds |
CDenFunctional | An abstract base class for density functionals |
CDenIntegrator | An abstract base class for integrating the electron density |
CDensityColorizer | |
CDensityFitting | Decomposition by density fitting with respect to some kernel |
CDensityFittingInfo | This class encapsulates objects needed to perform density fitting of a 4-center integral |
CDensityFittingParams | DensityFittingParams defines parameters used by DensityFittingRuntime and other runtime components to compute density fitting objects |
CDensityFittingRuntime | Smart runtime support for managing DensityFitting objects |
Cder_centersv3_t | |
CDerivCenters | DerivCenters keeps track the centers that derivatives are taken with respect to |
CDescribedClass | Classes which need runtime information about themselves and their relationship to other classes can virtually inherit from DescribedClass |
CDescribedClassProxy | Classes deriving from this are used to generate objects of DescribedClass type |
CDescribedXMLWritable | |
CDFCLHF | DFCLHF is a specialization of CLHF that uses a density-fitting FockBuild class for computing fock matrices |
CDFPUpdate | Used to specify a Davidson, Fletcher, and Powell hessian update scheme |
CDiagMolecularHessian | DiagMolecularHessian is an implementation of MolecularHessian that returns a hessian that is a diagonal matrix |
CDiagSCMatrix | The SymmSCMatrix class is the abstract base class for diagonal double valued matrices |
CDiagSCMatrixdouble | |
CDIIS | DIIS extrapolation |
CDipoleIntV3 | |
CDiscreteConnollyShape | DiscreteConnollyShape and ConnollyShape should produce the same result |
CDisplacements | Maps displacements in terms of symmetrized coordinates to property values |
CDistArray4 | DistArray4 contains a set of one or more distributed dense 4-index arrays |
CDistArray4_MemoryGrp | DistArray4_MemoryGrp handles transformed integrals held in memory by MemoryGrp |
►CDistArray4_MPIIOFile | DistArray4_MPIIOFile handles transformed integrals stored in a binary file accessed through MPI-IO |
CPairBlkInfo | |
CDistArray4_MPIIOFile_Ind | DistArray4_MPIIOFile_Ind handles transformed integrals stored in a binary file accessed through MPI-IO individual I/O routines |
CDistArray4_Node0File | DistArray4_Node0File handles transformed integrals stored in file on node 0 (file is a usual POSIX binary file) |
CDistArray4Creator | Creates new DistArray4 using TwoBodyFourCenterMOIntsRuntime and a vector of transform keys |
CDistArray4Dimensions | |
CDistDiagSCMatrix | Distributed DiagSCMatrix |
CDistFockBuildMatrix | |
CDistSCMatrix | Distributed SCMatrix |
CDistSCMatrixKit | The DistSCMatrixKit produces matrices that work in a many processor environment |
CDistSCMatrixListSubblockIter | |
CDistSCVector | |
►CDistShell | Distributes sets of shells either statically or dynamically |
CSharedData | This is used to store data that must be shared between all cooperating shell sets |
►CDistShellPair | Distributes shell pairs either statically or dynamically |
CSharedData | This is used to store data that must be shared between all cooperating shell pairs |
CDistSymmSCMatrix | Distributed SymmSCMatrix |
CDummySavableState | Useful as a dummy template argument |
►CEAVLMMap | |
Citerator | |
CEAVLMMapNode | |
CEdge | |
CEFCOpt | Implements eigenvector following as described by Baker in J |
CEfieldDotVectorData | |
CEfieldDotVectorIntV3 | |
CEfieldIntV3 | |
CEGH | Energy + gradient + hessian |
CElectronDensity | This is a Volume that computes the electron density |
CEmptyOrbitalSpace | This is an empty OrbitalSpace |
CEnergyMOOrder | Order by energy first, then by symmetry. EnergyCompare specifies the weak strict ordering of orbitals wrt energy |
CETraIn | Class ETraIn evaluates transfer and overlap matrix in the basis of monomer SCF wave functions |
CEulerMaclaurinRadialIntegrator | An implementation of a radial integrator using the Euler-Maclaurin weights and grid points |
CException | This is a std::exception specialization that records information about where an exception took place |
CExEnv | Used to find out about how the program is being run |
CExtendedHuckelWfn | This computes the extended Huckel energy and wavefunction |
CExtentData | |
CExtern_RefWavefunction | RefWavefunction specialization that is not an adaptor to a Wavefunction object |
CExternMOInfo | Reads MO information from a text file Note that the MO ordering in the external file may not be the same as in MPQC For example, irreducible representations may be ordered differently in different programs Thus MOs will be reordered to be consistent with MPQC rules, and a map from the native to MPQC representation will be provided so that other files produced by the external program can be interpreted |
CExternPT2R12 | ExternPT2R12 is a PT2R12 wave function computed from external MO info and 2-RDM |
CExternSpinFreeRDMOne | Reads 1-RDM from a text file |
CExternSpinFreeRDMTwo | Reads 2-RDM from a text file |
CFeatureNotImplemented | This is thrown when an attempt is made to use a feature that is not yet implemented |
CFEMO | Describes a simple the free-electron molecular orbital model that can be used to guess the lowest-energy orbital configuration |
CFermionBasicNCOper | Basic Nb-body number-conserving (nc) operator in sp representation |
CFermionBasicNCOper< 1, FString > | |
►CFermionOccupationBlockString | Block-"sparse" string represents occupancies of an arbitrarily-large set of states as a set of alternating unoccupied/occupied blocks |
CBlock | Continuous block of states of same occupancy |
CFermionOccupationDBitString | "dense" string represents occupancies of a set of Ns states by a bitstring |
CFermionOccupationNBitString | "dense" string represents occupancies of a set of Ns states by a fixed-width bitstring |
CFermionStringDenseSet | |
CFermionStringSparseSet | |
CFileGrp | The FileGrp abstract class provides a way of accessing distributed file in a parallel machine |
CFileOperationFailed | This is thrown when an operation on a file fails |
CFileRender | |
CFinDispMolecularGradient | Computes the molecular gradient by finite differences of energies |
CFinDispMolecularHessian | Computes the molecular hessian by finite displacements of gradients (or, if not available, energies) |
CFJT | "Old" intv3 code from Curt Computes F_j(T) using 6-th order Taylor interpolation |
CFjt | Evaluates the Boys function F_j(T) |
CFockBlocks | |
CFockBuild | Works with the FockBuildThread class to generate Fock matrices for both closed shell and open shell methods |
CFockBuildAM | |
CFockBuildAMG | |
CFockBuildCLHF | FockBuildCLHF is a specialization of CLHF that uses FockBuild class for computing fock matrices |
CFockBuildMatrix | |
CFockBuildOp | |
CFockBuildRuntime | Build Fock matrices using some combination of FockBuilder objects |
CFockBuildThread | Used to actually build the Fock matrix |
CFockBuildThread_F11_P11 | The FockBuildThread class is used to actually build the Fock matrix |
CFockBuildThread_F12_P33 | This is used to build the Fock matrix when none of the basis sets are equivalent |
CFockContribution | |
CFockDist | |
CFockDistDynamic | |
CFockDistDynamic2 | |
CFockDistDynamic4 | |
CFockDistribution | FockDistribution is a factory for constructing the desired FockDist specialization |
CFockDistStatic | |
CFockDistStatic2 | |
CFockDistStatic4 | |
CForceLink | This, together with ForceLinkBase, is used to force code for particular classes to be linked into executables |
CForceLinkBase | This, together with ForceLink, is used to force code for particular classes to be linked into executables |
CFreeData | |
CFullFermionStringSetBuild | Build all possible strings by distributing n particles in m states |
CFunction | Abstract base class that, given a set of coordinates, will compute a value and possibly a gradient and hessian at that point |
CG12NCLibint2 | G12NCLibint2 is a specialization of Int2eLibint2 that computes two-electron integrals specific to explicitly correlated methods which use Gaussian geminals (formulation without commutators) |
CG96XFunctional | Implements the Gill 1996 (G96) exchange functional |
►CGaussianBasisSet | Used describe a basis set composed of atomic gaussian orbitals |
CShell | Shell is a GaussianShell that is part of GaussianBasisSet, i.e. has a center on which it's centered |
CValueData | This holds scratch data needed to compute basis function values |
CGaussianBasisSetMap | A heavy-duty map from one GaussianBasisSet to another GaussianBasisSet |
CGaussianFit | GaussianFit<Function> is a fit of Function(x)*Weight(x) to N Gaussians on range [left,right] Valid Function and Weight are Unary Functions which take and return a double |
CGaussianShell | A shell of Gaussian functions |
CGaussLegendreAngularIntegrator | An implementation of an angular integrator using the Gauss-Legendre weights and grid points |
CGaussTriangleIntegrator | |
CGBuild | |
CGDIISOpt | |
►CGenericFockContribution | Much of the infrastructure needed by FockContribution specializations |
CJKBlock | |
CJLocator | |
CKLocator | |
CPBlock | |
CGenericPetiteList2 | This class provides a generalized 2-index petite list |
CGenericPetiteList4 | This class provides a generalized four index petite list |
CGetLongOpt | Parse command line options |
CGlobalCounter | Allows processes on the same SMP node to share a counter using SysV IPC semaphores |
CGlobalMsgIter | |
CGPetiteList2 | This class is an abstract base to a generalized 2-index petite list |
CGPetiteList4 | This class is an abstract base to a generalized four index petite list |
CGPetiteListFactory | Produces generalized 2 and 4-index petite list objects |
CGradDensityColorizer | |
CGrid | Defines a finite regular Carthesian grid |
CGrpArithmeticAndReduce | |
CGrpArithmeticOrReduce | |
CGrpArithmeticXOrReduce | |
CGrpCompareReduce | |
CGrpFunctionReduce | |
CGrpMaxReduce | |
CGrpMinReduce | |
CGrpProductReduce | |
CGrpReduce | |
CGrpSumReduce | |
CGRTLibint2 | GRTLibint2 is a specialization of Int2eLibint2 that computes two-electron integrals specific to linear R12 methods |
CGSGeneralEffH | |
CGSHighSpinEffH | |
CGTOInfo | Provides precomputed information about Gaussian basis functions |
CGuessMolecularHessian | GuessMolecularHessian is an implementation of MolecularHessian that estimates the hessian based on the internal coordinates |
Chash | |
CHCoreWfn | This is useful as an initial guess for other one body wavefunctions. Produces high-spin electron configurations |
CHessianUpdate | The HessianUpdate abstract class is used to specify a hessian update scheme |
CHSOSHF | HSOSHF is a Hartree-Fock specialization of HSOSSCF |
CHSOSHFContribution | Computes components of the Fock matrix necessary for high-spin open-shell calculations (e.g |
CHSOSKS | This provides a Kohn-Sham implementation for restricted-orbital high-spin open-shell systems |
CHSOSSCF | Base for classes implementing a self-consistent procedure for high-spin open-shell molecules |
CHSOSV1Erep1Qtr | |
CHundsFEMOSeeker | Finds the FEMO configuration that corresponds to the maximum multiplicity |
CHypercubeGMI | |
CHypercubeTopology | |
CIdentityKeyPermutation | |
CIdentityTransform | The IdentityTransform is a special case of NonlinearTransform were no transformation takes place |
Cignored_argument | |
CImplicitSurfacePolygonizer | |
CIndexRangeIterator | This is an abstract range of indices |
CInputError | This is thrown when invalid input is provided |
CInt1eLibint2 | Int1eLibint2 is used by OneBodyIntLibint2 and OneBodyDerivIntLibint2 to implement IntegralLibint2 |
CInt1eV3 | Int1eV3 is a class wrapper for the one body part of the C language IntV3 library |
CInt2eLibint2 | Int2eLibint2 is an interface to various specializations of two-electron integral evaluators implemented in Libint2 |
►CInt2eV3 | Int2eV3 is a class wrapper for the two body part of the C language IntV3 library |
Cstore_list | |
CIntCoor | The IntCoor abstract class describes an internal coordinate of a molecule |
CIntCoorGen | IntCoorGen generates a set of simple internal coordinates for a molecule |
CIntDescrFactory | |
CIntegral | The Integral abstract class acts as a factory to provide objects that compute one and two electron integrals |
CIntegralLibint2 | IntegralLibint2 computes integrals between Gaussian basis functions |
CIntegralSetDescr | IntegralSetDescr contains all information necessary to construct an IntEval object that computes a particular set of integrals using an Integral factory |
CIntegralV3 | IntegralV3 computes integrals between Gaussian basis functions |
CIntegrationWeight | An abstract base class for computing grid weights |
CIntEvalToOperSetType | |
CIntEvalToOperSetType< TwoBodyInt > | |
CIntEvalToOperSetType< TwoBodyThreeCenterInt > | |
CIntEvalToOperSetType< TwoBodyTwoCenterInt > | |
Cintlist_struct | |
CIntMolecularCoor | The IntMolecularCoor abstract class describes a molecule's coordinates in terms of internal coordinates |
CIntParams | This class passes optional operator parameters |
CIntParamsG12 | Used to pass params to Integral::g12() |
CIntParamsOrigin | Passes params to Integral::dipole() and other factory methods which need r information |
CIntParamsVoid | Passes params to Integral::electron_repulsion() and other factory methods which do not need parameters |
CIntV3Arraydouble2 | |
CIntV3Arraydouble3 | |
CIntV3Arraydoublep2 | |
CIntV3Arraydoublep3 | |
CIntV3Arraydoublep4 | |
CIntV3Arrayint3 | |
CIntV3Arrayint4 | |
Cip_cwk_stack_struct | |
Cip_keyword_tree_list_struct | |
Cip_keyword_tree_struct | |
Cip_string_list_struct | |
CIPV2 | |
CIrreducibleRepresentation | Information associated with a particular irreducible representation of a point group |
CIsosurfaceGen | |
CISphericalTransform | This describes a solid harmonic to Cartesian transform |
CISphericalTransformLibint2 | |
CISphericalTransformV3 | |
CIterableBasisElementData | |
CKeyPermutation | |
CKeySymmetry | |
CKeyTransposition | |
CKeyVal | |
CKeyValValue | Represents the value of a keyword |
CKeyValValueboolean | Represents a boolean value |
CKeyValValuechar | Represents a char value |
CKeyValValuedouble | Represents a double value |
CKeyValValuefloat | Represents a float value |
CKeyValValueint | Represents an int value |
CKeyValValuelong | Represents a long value |
CKeyValValuepchar | Represents a pointer to char value (deprecated, use KeyValValuestring) |
CKeyValValueRefDescribedClass | Represents a Ref<DescribedClass> value |
CKeyValValuesize | Represents a size_t value |
CKeyValValuestring | Represents a std::string value |
CKeyword | |
CLAMBDA_CCSD_T1 | |
CLAMBDA_CCSD_T2 | |
CLAMBDA_CCSDPR12_T1 | |
CLAMBDA_CCSDPR12_T2 | |
CLazyTensor | Tile of a DIM-order tensor that's "evaluated" when needed by calling ElementGenerator({i0, i1, i2, .... i_DIM-1}) |
CLCorr | A base class for local correlation methods |
CLebedevLaikovIntegrator | An implementation of a Lebedev angular integrator |
CLevelShift | |
CLibint2StaticInterface | |
CLibr12StaticInterface | |
CLimitExceeded | This is thrown when a limit is exceeded |
CLineOpt | The LineOpt abstract class is used to perform one dimensional optimizations |
CLinIPSimpleCo | Describes an in-plane component of a linear bend internal coordinate of a molecule |
CLinKListGroup | |
CLinOPSimpleCo | Describes an out-of-plane component of a linear bend internal coordinate of a molecule |
CLMP2 | Computes the local second order perturbation theory energy |
CLocalCLHFContribution | |
CLocalCLHFEnergyContribution | |
CLocalCLHFGradContribution | |
CLocalCLKSContribution | |
CLocalCLKSEnergyContribution | |
CLocalDiagSCMatrix | Local DiagSCMatrix |
CLocalGBuild | |
CLocalHSOSContribution | |
CLocalHSOSEnergyContribution | |
CLocalHSOSGradContribution | |
CLocalHSOSKSContribution | |
CLocalHSOSKSEnergyContribution | |
CLocalLBGBuild | |
CLocalOSSContribution | |
CLocalOSSEnergyContribution | |
CLocalOSSGradContribution | |
CLocalSCMatrix | |
CLocalSCMatrixKit | The LocalSCMatrixKit produces matrices that work in a single processor environment |
CLocalSCVector | |
CLocalSymmSCMatrix | Local SymmSCMatrix |
CLocalTBGrad | |
CLocalTCContribution | |
CLocalTCEnergyContribution | |
CLocalTCGradContribution | |
CLocalUHFContribution | |
CLocalUHFEnergyContribution | |
CLocalUHFGradContribution | |
CLocalUKSContribution | |
CLocalUKSEnergyContribution | |
CLog2Bounds | Computes log2 bounds |
CLSDACFunctional | An abstract base class for local correlation functionals |
CLSelectBasisSet | Used to select shells by angular momentum from a mother basis |
CLYPCFunctional | Implements the Lee, Yang, and Parr functional |
CMachineTopology | |
CManyBodyWavefunction | ManyBodyWavefunction is a Wavefunction obtained from a reference OneBodyWavefunction (its orbitals or more) |
CMaskedOrbitalSpace | This is an OrbitalSpace produced from an existing one by masking out some Orbitals |
Cmat3 | |
Cmat4 | |
CMaterial | |
CMaxIterExceeded | This is thrown when an iterative algorithm attempts to use more iterations than allowed |
CMBPT2 | Implements several second-order perturbation theory methods |
CMBPT2_R12 | Implements several R12 second-order Moeller-Plesset perturbation theory methods |
CMCSearch | This performs line searches with cubic steps |
CMemAllocFailed | This is thrown when a memory allocation fails |
CMemoryDataRequest | This is a help class used by ActiveMsgMemoryGrp |
CMemoryDataRequestQueue | This is a help class used by ActiveMsgMemoryGrp |
CMemoryGrp | The MemoryGrp abstract class provides a way of accessing distributed memory in a parallel machine |
CMemoryGrpBuf | The MemoryGrpBuf class provides access to pieces of the global shared memory that have been obtained with MemoryGrp |
CMemoryGrpRegion | The MemoryGrpRegion is a MemoryGrp proxy to a region of a MemoryGrp |
CMemoryIter | This iterates through data in a global array |
Cmessage_struct | |
►CMessageGrp | The MessageGrp abstract class provides a mechanism for moving data and objects between nodes in a parallel machine |
CMessageHandle | |
CMessageInfo | |
CMOIntsRuntime | MOIntsRuntime provides runtime support for computing 1-body and 2-body (2-, 3-, and 4-center) MO-basis integrals (with or without density fitting) |
►CMOIntsTransform | |
CStoreMethod | Describes the method of storing transformed MO integrals |
CMOIntsTransformFactory | MOIntsTransformFactory is a factory that produces MOIntsTransform objects |
CMOLagrangian | |
CMolcasPT2R12 | Interface between Molcas and MPQC to perform CASPT2F12 calculations |
CMOLDEN_ExternReadMOInfo | Reads MO information from a text MOLDEN file |
CMolecularCoor | The MolecularCoor abstract class describes the coordinate system used to describe a molecule |
CMolecularEnergy | The MolecularEnergy abstract class inherits from the Function class |
CMolecularFormula | Used to calculate the molecular formula of a Molecule |
CMolecularFragment | MolecularFragment is a Molecule that is a fragment of another Molecule object |
CMolecularFrequencies | Used to compute the molecular frequencies and thermodynamic information |
CMolecularGradient | MolecularGradient is an abstract class that computes a molecule's first derivatives of the energy with respect to changes in the nuclear coordinates |
CMolecularHessian | MolecularHessian is an abstract class that computes a molecule's second derivatives of the energy with respect to changes in the nuclear coordinates |
CMolecularOrbitalAttributes | MO is irrep, energy, occupation number |
CMolecularOrbitalMask | Mask out first n MOs in the order defined by Compare. By default mask the n lowest-energy MOs |
CMolecularSpinOrbitalAttributes | Same as MolecularOrbitalAttributes, plus spin |
CMolecule | Information about molecules |
CMoleculeColorizer | |
CMolEnergyConvergence | |
CMolFreqAnimate | |
CMOPairIter | MOPairIter gives the ordering of orbital pairs |
CMOPairIterFactory | This class produces MOPairIter objects |
CMP2BasisExtrap | |
CMP2R12Energy | Class MP2R12Energy is the object that computes and maintains MP2-R12 energies |
CMP2R12Energy_Diag | The class MP2R12Energy_Diag is an implementation of MP2R12Energy that supports Ten-no's diagonal orbital-invariant ansatz for closed and open-shells |
CMP2R12Energy_SpinOrbital | The class MP2R12Energy_SpinOrbital is the original implementation of MP2R12Energy It supports only the standard orbital-invariant ansatz and the full set of features of R12Technology |
CMP2R12EnergyUtil_base | Class MP2R12EnergyUtil_base is the abstract interface to utility functions used by MP2R12Energy derivatives |
CMP2R12EnergyUtil_Diag | |
CMP2R12EnergyUtil_Diag_DifferentSpin | Class MP2R12EnergyUtil provides some misc functions to operate on (blocked) ijxy and xyxy matrices |
CMP2R12EnergyUtil_Diag_SameSpin | |
CMP2R12EnergyUtil_Nondiag | |
►CMPIMessageGrp | Concrete implementation of MessageGrp that uses the MPI 1 library |
CMessageHandleData | |
►CMPQCIn | Converts MPQC simple input to object-oriented input |
CBasis | |
CMPQCInDatum | |
CMPQCInit | This helper class simplifies initialization of MPQC |
CmPW91XFunctional | Implements a modified 1991 Perdew-Wang exchange functional |
CMsgMemoryGrp | A MsgMemoryGrp that initializes its data using a messagegrp |
CMsgStateBufRecv | The MsgStateBufRecv is an abstract base class that buffers objects sent through a MessageGrp |
CMsgStateRecv | The MsgStateRecv is an abstract base class that receives objects from nodes in a MessageGrp |
CMsgStateSend | The MsgStateSend is an abstract base class that sends objects to nodes in a MessageGrp |
CMTensor | Tensor metadata is implicit; MTensor is Tensor + metadata |
CMTMPIMemoryGrp | This MemoryGrp class requires a MT-safe MPI implementation |
CMultiThreadTimer | |
CNBodyIntEval | This is an abstract base type for classes that compute integrals of general N-body operators described by OperDescr |
CNBodyIntIter | |
CNCAccResult | This associates a result non-class datum with an accuracy |
CNCentersToIntDescr | |
CNCentersToIntDescr< 1, 1 > | |
CNCentersToIntDescr< 2, 1 > | |
CNCentersToIntDescr< 2, 2 > | |
CNCentersToIntDescr< 3, 2 > | |
CNCentersToIntDescr< 4, 2 > | |
CNCResult | This is similar to Result, but can be used with non-class types |
CNElFunctional | The NElFunctional computes the number of electrons |
CNewP86CFunctional | |
CNewtonOpt | Implements Newton method |
CNonblockedOrbitalSpace | This is an OrbitalSpace produced from an existing one by getting rid of the blocking |
CNonlinearTransform | Transforms between two nonlinear coordinate systems |
CNonreentrantUncappedTorusHoleShape | |
COBWfnRDMCumulantTwo | OBWfnRDMCumulantTwo is the cumulant of OBWfnRDMTwo |
COBWfnRDMOne | OBWfnRDMOne is a 1-RDM from a OneBodyWavefunction |
COBWfnRDMTwo | OBWfnRDMTwo is a 2-RDM from a OneBodyWavefunction |
COneBody3IntOp | |
COneBodyDerivInt | OneBodyDerivInt is an abstract base class for objects that compute one body derivative integrals |
COneBodyDerivIntV3 | This implements one body derivative integrals in the IntV3 library |
COneBodyFockMatrixBuilder | Builds the one-body part of the Fock matrix in AO basis |
COneBodyInt | OneBodyInt is an abstract base class for objects that compute integrals between two basis functions |
COneBodyIntEvalType | Returns the type of the evaluator for evaluating this set of two-body integrals |
COneBodyIntEvalType< 1 > | |
COneBodyIntEvalType< 2 > | |
COneBodyIntIter | |
COneBodyIntLibint2 | This implements most one body integrals in the Libint2 library |
COneBodyIntOp | |
COneBodyIntParamsType | Which parameter set needed to specify the operator set? |
COneBodyIntParamsType< OneBodyOperSet::ddphi > | |
COneBodyIntParamsType< OneBodyOperSet::dphi > | |
COneBodyIntParamsType< OneBodyOperSet::h > | |
COneBodyIntParamsType< OneBodyOperSet::mu > | |
COneBodyIntParamsType< OneBodyOperSet::p4 > | |
COneBodyIntParamsType< OneBodyOperSet::phi > | |
COneBodyIntParamsType< OneBodyOperSet::pVp > | |
COneBodyIntParamsType< OneBodyOperSet::q > | |
COneBodyIntParamsType< OneBodyOperSet::T > | |
COneBodyIntParamsType< OneBodyOperSet::V > | |
COneBodyIntTraits | Traits of a set of one-body integrals |
COneBodyIntType | |
COneBodyIntType< 1 > | |
COneBodyIntType< 2 > | |
COneBodyIntV3 | This implements most one body integrals in the IntV3 library |
COneBodyNCenterIntDescr | Implements descriptors for various two-body evaluators |
COneBodyOneCenterDerivInt | OneBodyOneCenterDerivInt is an abstract base class for objects that compute one body derivative integrals on a single center |
COneBodyOneCenterInt | OneBodyOneCenterInt is an abstract base class for objects that compute integrals between two basis functions |
COneBodyOneCenterWrapper | |
COneBodyOper | Describes one-body operators |
COneBodyOperDescr | Describes permutational properties (hermiticity) of one-body operators |
COneBodyOperSet | Describes sets of one-body operator |
COneBodyOperSetDescr | Runtime version of OneBodyOperSetProperties |
COneBodyOperSetProperties | Describes sets of two-body operators ( |
COneBodyOperSetProperties< OneBodyOperSet::ddphi > | |
COneBodyOperSetProperties< OneBodyOperSet::dphi > | |
COneBodyOperSetProperties< OneBodyOperSet::h > | |
COneBodyOperSetProperties< OneBodyOperSet::mu > | |
COneBodyOperSetProperties< OneBodyOperSet::p4 > | |
COneBodyOperSetProperties< OneBodyOperSet::phi > | |
COneBodyOperSetProperties< OneBodyOperSet::pVp > | |
COneBodyOperSetProperties< OneBodyOperSet::q > | |
COneBodyOperSetProperties< OneBodyOperSet::S > | |
COneBodyOperSetProperties< OneBodyOperSet::T > | |
COneBodyOperSetProperties< OneBodyOperSet::V > | |
COneBodySODerivInt | OneBodySODerivInt computes two-center one-electron integrals in a symmetry-adapted basis |
COneBodySOInt | OneBodySOInt computes two-center one-electron integrals in a symmetry-adapted basis |
COneBodyWavefunction | A OneBodyWavefunction is a MolecularEnergy that solves an effective one-body problem |
COOGLRender | |
COperatorDescr | For an operator (e.g |
COptimize | Abstract base class for classes that find the extreme points of Function's |
COptionalRefParameter | |
COrbital | |
COrbitalSpace | Class OrbitalSpace describes a range of orbitals that are linear combinations of Gaussian basis functions (e.g |
COrbitalSpaceUnion | This is a union of two OrbitalSpaces s1 and s2 |
COrderedOrbitalSpace | This is an OrbitalSpace ordered according to the Order type |
COrderedShellList | |
COrderedSpinOrbitalSpace | Same as OrderedOrbitalSpace, except for spin-orbitals |
COSSHF | Hartree-Fock-like wave function for open-shell singlet electronic configurations |
COSSSCF | SCF implementation for open-shell singlet electronic configurations |
COutSimpleCo | |
COverlapOrthog | This class computes the orthogonalizing transform for a basis set |
CP86CFunctional | Implements the Perdew 1986 (P86) correlation functional |
CParallelRegionTimer | This is a parallel-away derivative of RegionTimer |
CParameter | |
CParamsRegistry | This is a singleton registry that holds IntParams objects |
CParentClass | Gives one parent class of a class |
CParentClasses | Gives a list of parent classes of a class |
CParenthesis2q | |
CParenthesis2t | |
CParenthesis2tNum | PTNum is the base class for the numerator in various (2)T/(2)Q models |
CParsedDensityFittingKey | Parsed representation of a string key that represents fitting of a product of space1 and space2 into fspace |
CParsedKeyVal | |
CParsedOneBodyIntKey | Parsed representation of a string key that represents a set of one-body integrals |
CParsedOneBodyOperSetKey | Parsed representation of a string key that represents a one-body operator set (OneBodyOperSet + associated parameters) |
►CParsedOrbitalSpaceKey | Parses keys of OrbitalSpace |
Cexception | |
►CParsedTransformedOrbitalSpaceKey | Parses keys of a "transformed" OrbitalSpace |
Cexception | |
CParsedTwoBodyFourCenterIntKey | Parsed representation of a string key that represents a set of 4-center 2-body integrals |
CParsedTwoBodyMOIntsKeyInvolvesSpace | |
CParsedTwoBodyMOIntsKeyInvolvesSpace< 2 > | |
CParsedTwoBodyMOIntsKeyInvolvesSpace< 3 > | |
CParsedTwoBodyMOIntsKeyInvolvesSpace< 4 > | |
CParsedTwoBodyOperSetKey | Parsed representation of a string key that represents a two-body operator set (TwoBodyOperSet + associated parameters) |
CParsedTwoBodyThreeCenterIntKey | Parsed representation of a string key that represents a set of 3-center 2-body integrals |
CParsedTwoBodyTwoCenterIntKey | Parsed representation of a string key that represents a set of 2-center 2-body integrals |
CParticleHoleOrbitalAttributes | Describes particle-hole attributes of orbitals |
CPBECFunctional | Implements the Perdew-Burke-Ernzerhof (PBE) correlation functional |
CPBEXFunctional | Implements the Perdew-Burke-Ernzerhof (PBE) exchange functional |
CPermutedDensityFitting | Computes density fitting for |ij) density from fitting of |ji) DensityFitting |
CPetiteList | PetiteList is a petite list (see Dupuis & King, IJQC 11,613,(1977) ) that can be used for constructing symmetry-adapted basis functions (`‘symmetry orbitals’', SO for short) as well as transforming operators and functions from AO to SO basis, and vice versa |
CPipekMezeyLocalization | Performs a Pipek-Mezey orbital localization |
CPointChargeData | |
CPointChargeIntV3 | |
CPointGroup | Really a place holder for a CharacterTable |
►CPointInputData | Contains data needed at each point by a DenFunctional |
CSpinData | |
CPointOutputData | Contains data generated at each point by a DenFunctional |
CPool | |
CPoolData | |
CPopulatedOrbitalSpace | PopulatedOrbitalSpace is an OrbitalSpace populated with a density |
CPowellUpdate | Used to specify a Powell hessian update |
CPrefixKeyVal | |
Cprim_pair_t | |
CPrimPairsLibint2 | PrimPairsLibint2 contains primitive pair data |
CProcFileGrp | The ProcFileGrp concrete class provides an implementation of FileGrp for a single processor |
CProcMemoryGrp | The ProcMemoryGrp concrete class provides an implementation of MemoryGrp for a single processor |
CProcMessageGrp | ProcMessageGrp provides a concrete specialization of MessageGrp that supports only one node |
CProcThreadGrp | Privides a concrete thread group appropriate for an environment where there is only one thread |
Cproduct_iterator | |
CProgrammingError | This is thrown when a situations arises that should be impossible |
Cproperty | Helper class to connect a 'property' in a c++ class to getter/setter methods |
CPsiCC | PsiCC is a Psi coupled cluster wave function |
CPsiCC2 | PsiCC2 is a concrete implementation of Psi ground-state CC2 wave function |
CPsiCC3 | PsiCC3 is a concrete implementation of Psi ground-state CC3 wave function |
CPsiCC3_PT2R12 | PsiCC3_PT2R12 is a concrete implementation of the ground-state method |
CPsiCC_PT2R12 | PsiCC_PT2R12 is used to implement methods |
CPsiCCSD | PsiCCSD is a concrete implementation of Psi CCSD wave function |
CPsiCCSD_PT2R12 | PsiCCSD_PT2R12 is a concrete implementation of the method |
CPsiCCSD_PT2R12T | PsiCCSD_PT2R12T is a concrete implementation of the method |
CPsiCCSD_T | PsiCCSD_T is a concrete implementation of Psi CCSD(T) wave function |
CPsiChkpt | PsiChkpt know to read data from Psi checkpoint file and convert it to conform to the representations expected in MPQC |
CPsiCLHF | PsiCLHF is a concrete implementation of Psi RHF wave function |
CPsiCorrWavefunction | PsiCorrWavefunction is a Psi correlated wave function |
CPsiEffH | |
CPsiExEnv | PsiExEnv specifies a Psi execution environment |
CPsiFile11 | PsiFile11 is a Psi gradient file |
CPsiHSOSHF | PsiHSOSHF is a concrete implementation of Psi ROHF wave function |
CPsiInput | PsiInput is a Psi input file |
CPsiRASCI | PsiRASCI is a general (RAS) CI PsiWavefunction |
CPsiRASCI_RefWavefunction | RefWavefunction specialization for a general restricted-active-space multiconfiguration wave function |
CPsiRASSCF | PsiRASSCF is a type of a PsiRASCI wavefunction that implements orbital optimization |
CPsiRDMOne | PsiRDMOne is a 1-RDM from a PsiWavefunction |
CPsiRDMTwo | PsiRDMTwo is a 2-RDM from a PsiWavefunction |
CPsiSCF | PsiSCF is an abstract base for all Psi SCF wave functions |
CPsiSCF_RefWavefunction | RefWavefunction specialization initialized with a PsiSCF wave function |
CPsiSpinFreeRDMOne | PsiSpinFreeRDMOne is a spin-free 1-RDM from a PsiWavefunction |
CPsiSpinFreeRDMTwo | PsiRDMTwo is a spin-free 2-RDM from a PsiWavefunction |
CPsiUHF | PsiUHF is a concrete implementation of Psi UHF wave function |
CPsiWavefunction | PsiWavefunction is an abstract base for all Psi wave functions |
CPT2R12 | PT2R12: a universal spin-free second-order R12 correction |
CPthreadThreadGrp | Privides a concrete thread group appropriate for an environment where pthreads is available |
CPTNum | PTNum is the base class for the numerator in various (T) models |
CPumaThreadGrp | Privides a concrete thread group appropriate for the intel teraflops machine |
CPW86XFunctional | Implements the Perdew-Wang 1986 (PW86) Exchange functional |
CPW91CFunctional | The Perdew-Wang 1991 correlation functional computes energies and densities using the designated local correlation functional |
CPW91XFunctional | The Perdew-Wang 1991 exchange functional computes energies and densities using the designated local correlation functional |
CPW92LCFunctional | Implements the PW92 local (LSDA) correlation term |
CPZ81LCFunctional | Implements the PZ81 local (LSDA) correlation functional |
CQNewtonOpt | The QNewtonOpt implements a quasi-Newton optimization scheme |
CR12Amplitudes | R12Amplitudes gives the amplitudes of some R12-ansatz-related terms in wave function |
CR12EnergyIntermediates | The class R12EnergyIntermediates is the front-end to R12 intermediates |
CR12IntEval | R12IntEval is the top-level class which computes intermediates occuring in R12 theories |
►CR12Technology | R12Technology describes technical features of the R12 approach |
CCorrelationFactor | CorrelationFactor is a set of one or more two-particle functions of the interparticle distance |
CCorrParamCompare | Compares CorrelationParamaters corresponding to IntParam |
CG12CorrelationFactor | G12CorrelationFactor stands for Gaussian geminals correlation factor, usable with methods that require commutator integrals |
CG12NCCorrelationFactor | G12NCCorrelationFactor stands for Gaussian geminals correlation factor, usable with methods that do not require commutator integrals; this is more for temporary tests or quick implementation |
CGeminalDescriptor | |
CGeminalDescriptorFactory | |
CNullCorrelationFactor | NullCorrelationFactor stands for no correlation factor; only for test |
CR12Ansatz | R12Ansatz specifies the manner in which the R12 geminals are constructed |
CR12CorrelationFactor | R12CorrelationFactor stands for no correlation factor |
CR12TwoBodyIntKeyCreator | Creates R12TwoBodyIntKey for the given CorrelationFactor |
CR12WavefunctionWorld | Class R12WavefunctionWorld describes the environment of a Wavefunction implementing an R12 method |
CRadialAngularIntegrator | An implementation of an integrator using any combination of a RadialIntegrator and an AngularIntegrator |
CRadialIntegrator | An abstract base class for radial integrators |
CRangeCreator | RangeCreator<T> is Functor which can be used up to n times to create objects of type T |
CRangeLock | |
CRangeLockItem | |
CRDM | RDM<R> is a reduced density matrix of rank R |
CRDM< Zero > | This specialization is needed to make RDM<R>::rdm_m_1() work |
CRDMAMemoryGrp | The RDMAMemoryGrp abstract class specializes the MsgMemoryGrp class |
CRDMCumulant | RDMCumulant<R> is a reduced density matrix cumulant of rank R |
CReadMolecularHessian | ReadMolecularHessian is an implementation of MolecularHessian that reads the hessian from a file |
CRedundantCartesianIter | RedundantCartesianIter objects loop through all possible combinations of a given number of axes |
CRedundantCartesianIterCCA | |
CRedundantCartesianIterGAMESS | |
CRedundantCartesianIterV3 | |
CRedundantCartesianSubIter | Like RedundantCartesianIter, except a, b, and c are fixed to a given value |
CRedundantCartesianSubIterCCA | |
CRedundantCartesianSubIterGAMESS | |
CRedundantCartesianSubIterV3 | |
CRedundMolecularCoor | Redundant set of simple internal coordinates |
Creentrant_auto_time_accumulator | |
Creentrant_time_accumulator_factory | |
CReentrantUncappedTorusHoleShape | |
CRef | A template class that maintains references counts |
CRefBase | Provides a few utility routines common to all Ref template instantiations |
CRefCount | The base class for all reference counted objects |
CRefDiagSCMatrix | Smart pointer to an DiagSCMatrix specialization |
CRefObjectEqual | This functor can be used as a binary predicate for standard algorithms |
CRefSCDimension | Smart pointer to an SCDimension specialization |
CRefSCMatrix | Smart pointer to an SCMatrix specialization |
CRefSCVector | Smart pointer to an SCVector specialization |
CRefSymmSCMatrix | Smart pointer to an SCSymmSCMatrix specialization |
CRefSymmSCMatrixEqual | This functor compares RefSymmSCMatrix objects |
CRefWavefunction | RefWavefunction represents the reference wave function (or, more generally, a state) used as a starting point for the introduction of electron correlation |
CRefWavefunctionFactory | This factory produces the RefWavefunction that corresponds to the type of ref object |
CRegionTimer | Used to record the time spent in a section of code |
►CRegistry | Registry wraps std::map and can be policy-configured to act as a Singleton or a regular object |
Cnot_found | |
CRender | |
CRenderedBallMolecule | |
CRenderedMolecularSurface | |
CRenderedMolecule | |
CRenderedObject | |
CRenderedObjectSet | |
CRenderedPolygons | |
CRenderedPolylines | |
CRenderedSphere | |
CRenderedStickMolecule | |
CReplDiagSCMatrix | Replicated DiagSCMatrix |
CReplFockBuildMatrix | |
CReplSCMatrix | |
CReplSCMatrixKit | The ReplSCMatrixKit produces matrices that work in a many processor environment |
CReplSCMatrixListSubblockIter | |
CReplSCVector | |
CReplSymmSCMatrix | Replicated SymmSCMatrix |
CResult | Result are members of Compute specializations that keep track of whether or not a particular result should be computed or if it has already been computed |
CResultInfo | This is a base class for all of Compute's result types |
CRunnable | DescribedClass with a pure virtual run member |
CSavableState | Base class for objects that can save/restore state |
CSavableStateProxy | |
CScaledTorsSimpleCo | Describes an scaled torsion internal coordinate of a molecule |
CSCBlockInfo | SCBlockInfo contains blocking information for the SCDimension class |
CSCDimension | Used to determine the size and blocking of matrices |
CSCElement | |
CSCElementAccumulateDiagSCMatrix | |
CSCElementAccumulateSCMatrix | |
CSCElementAccumulateSCVector | |
CSCElementAccumulateSymmSCMatrix | |
CSCElementAssign | |
CSCElementBinaryPredicateAdapter | Adapts a binary predicate that acts on SCElement::value_type |
CSCElementDAXPY | Does |
CSCElementDestructiveProduct | Does |
CSCElementDot | |
CSCElementFindExtremum | Searches each range in IterationRanges for element i so that there is no element j in that Range for which Op(i,j) == true |
CSCElementInvert | |
CSCElementKNorm | Computes k-norm of matrix |
CSCElementMaxAbs | |
CSCElementMinAbs | |
CSCElementOp | Objects of class SCElementOp are used to perform operations on the elements of matrices |
CSCElementOp2 | Very similar to the SCElementOp class except that pairs of blocks are treated simultaneously |
CSCElementOp3 | Very similar to the SCElementOp class except that a triplet of blocks is treated simultaneously |
CSCElementRandomize | |
CSCElementScalarProduct | Evaluates |
CSCElementScale | |
CSCElementScaleDiagonal | |
CSCElementShiftDiagonal | |
CSCElementSquareRoot | |
CSCElementSum | |
CSCException | This is a sc::Exception specialization that keeps track of the ClassDesc for the MPQC object from which it is thrown, and optional sc::Debugger::Backtrace object |
CSCExtrapData | SCExtrapData hold the data to be extrapolated needed by SelfConsistentExtrapolation |
CSCExtrapError | SCExtrapError holds the error data needed by SelfConsistentExtrapolation |
CSCF | Base for all classes that use a self-consistent field procedure to solve an effective one body problem |
CSCFEnergy | |
CSCFIterationData | |
CSCFIterationLogger | |
CSCFormIO | This utility class is used to print only on node 0 and to provide attractive indentation of output |
CSCMatrix | Abstract base class for general double valued n by m matrices |
CSCMatrix3 | |
CSCMatrixBlock | SCMatrixBlock is the base clase for all types of blocks that comprise matrices and vectors |
CSCMatrixBlockIter | Used to described iterates that loop through the elements in a block |
CSCMatrixBlockList | |
CSCMatrixBlockListIter | |
CSCMatrixBlockListLink | |
CSCMatrixCompositeSubblockIter | |
CSCMatrixDiagBlock | The SCMatrixDiagBlock describes a diagonal piece of a matrix |
CSCMatrixDiagBlockIter | |
CSCMatrixDiagSubBlock | The SCMatrixDiagSubBlock describes a diagonal subblock of a matrix |
CSCMatrixDiagSubBlockIter | |
CSCMatrixdouble | |
CSCMatrixIterationRanges | |
CSCMatrixJointSubblockIter | |
CSCMatrixKit | The SCMatrixKit abstract class acts as a factory for producing matrices |
CSCMatrixListSubblockIter | |
CSCMatrixLTriBlock | The SCMatrixLTriBlock describes a triangular piece of a matrix |
CSCMatrixLTriBlockIter | |
CSCMatrixLTriSubBlock | The SCMatrixLTriSubBlock describes a triangular subblock of a matrix |
CSCMatrixLTriSubBlockIter | |
CSCMatrixNullSubblockIter | |
CSCMatrixRectBlock | The SCMatrixRectBlock describes a rectangular piece of a matrix |
CSCMatrixRectBlockIter | |
CSCMatrixRectSubBlock | The SCMatrixRectSubBlock describes a rectangular piece of a matrix |
CSCMatrixRectSubBlockIter | |
CSCMatrixSimpleSubblockIter | |
CSCMatrixSubblockIter | Objects of class SCMatrixSubblockIter are used to iterate through the blocks of a matrix |
Cscprintf | This class allows printf -like output to be sent to an ostream |
CSCVector | Abstract base class for double valued vectors |
CSCVector3 | 3-element version of SCVector |
CSCVectordouble | |
CSCVectorSimpleBlock | The SCVectorSimpleBlock describes a piece of a vector |
CSCVectorSimpleBlockIter | |
CSCVectorSimpleSubBlock | The SCVectorSimpleSubBlock describes a subblock of a vector |
CSCVectorSimpleSubBlockIter | |
CSD_RefWavefunction | RefWavefunction specialization for a single-determinant wave function |
CSelfConsistentExtrapolation | The SelfConsistentExtrapolation abstract class is used to iteratively solve equations requiring a self consistent solution, such as, |
CSetIntCoor | Describes a set of internal coordinates |
CShape | A Shape is a Volume represents an 3D solid |
Cshell_block_iterator | |
CShellBlockData | |
CShellBlockIterator | |
CShellBlockSkeleton | |
CShellData | |
CShellDataWithValue | |
CShellExtent | |
CShellIndexWithValue | Binds an integer index + real annotation, e.g. Shell index + associated operator norm |
CShellPairIter | |
CShellPairLibint2 | ShellPairLibint2 is an interface to PrimPairsLibint2 |
CShellPairsLibint2 | ShellPairsLibint2 contains primitive pair data for all shell pairs formed from a pair of basis sets |
CShellQuartetIter | |
CShellRotation | Compute the transformation matrices that maps a set of Cartesian functions to another set of Cartesian functions in a rotated coordinate system |
CShmMemoryGrp | The ShmMemoryGrp concrete class provides an implementation of MsgMemoryGrp |
CSimpleCo | The SimpleCo abstract class describes a simple internal coordinate of a molecule |
CSingleReference_R12Intermediates | SingleReference_R12Intermediates computes R12/F12 intermediates using MPQC3 runtime |
CSlaterXFunctional | Implements the Slater exchange functional |
CSO | |
CSO_block | |
CSOBasis | A SOBasis object describes the transformation from an atomic orbital basis to a symmetry orbital basis |
CSOTransform | SOTransform maintains a list of AO shells that are be used to compute the SO |
CSOTransformFunction | SOTransformShell describes how an AO function contributes to an SO function in a particular SO shell |
CSOTransformShell | SOTransformShell maintains a list of AO functions contribute to an SO function in a particular SO shell |
CSpatialMOPairIter | SpatialMOPairIter gives the ordering of pairs of spatial orbitals |
CSpatialMOPairIter_eq | SpatialMOPairIter_eq gives the ordering of same-spin and different-spin orbital pairs if both orbitals of the pairs are from the same space |
CSpatialMOPairIter_neq | SpatialMOPairIter_neq gives the ordering of pairs of spatial orbitals from different spaces |
CSphereShape | |
CSphericalTransform | This is a base class for a container for a sparse Cartesian to solid harmonic basis function transformation |
CSphericalTransformComponent | This is a base class for a container for a component of a sparse Cartesian to solid harmonic basis function transformation |
CSphericalTransformComponentLibint2 | |
CSphericalTransformComponentV3 | |
CSphericalTransformIter | This iterates through the components of a SphericalTransform |
CSphericalTransformLibint2 | |
CSphericalTransformV3 | |
CSpinFreeRDM | SpinFreeRDM<R> is a spin-free reduced density matrix of rank R |
CSpinFreeRDM< Zero > | This specialization is needed to make SpinFreeRDM<R>::rdm_m_1() work |
CSpinMOPairIter | SpinMOPairIter iterates over pairs of spinorbitals |
CSpinOrbitalPT2R12 | SpinOrbitalPT2R12: a universal second-order R12 correction |
CSplitBasisSet | Used to split a basis set's contractions into multiple shells |
CSSAccResult | This associates a result datum with an accuracy |
CStack | |
CStateClassData | |
CStateIn | |
CStateInBin | |
CStateInData | |
CStateInFile | |
CStateInText | |
CStateOut | |
CStateOutBin | |
CStateOutData | |
CStateOutFile | |
CStateOutText | |
CStateRecv | StateRecv is a concrete specialization of MsgStateRecv that does the receive part of point to point communication in a MessageGrp |
CStateSend | StateSend is a concrete specialization of MsgStateSend that does the send part of point to point communication in a MessageGrp |
CStdDenFunctional | Used to construct the standard density functionals |
CSteepestDescentOpt | |
CStreSimpleCo | Describes an stretch internal coordinate of a molecule |
CStringKeyVal | |
CStringReplacementListIterator | Iterates over strings obtained by rank R replecement from a given string |
CSumAccumH | This specialization of AccumHNull does nothing |
CSumDenFunctional | The SumDenFunctional computes energies and densities using the a sum of energy density functions method |
CSumIntCoor | SumIntCoor is used to construct linear combinations of internal coordinates |
CSumMolecularEnergy | Linear combination of MolecularEnergy objects |
CSuperpositionOfAtomicDensities | SuperpositionOfAtomicDensities is a OneBodyWavefunction useful as a guess for other OneBodyWavefunction objects |
CSymmetryMOOrder | Order by symmetry first, then by energy, then by occ num |
CSymmetryOperation | 3 by 3 matrix representation of a symmetry operation, such as a rotation or reflection |
CSymmMolecularCoor | Derives from IntMolecularCoor |
CSymmOneBodyIntIter | Iterator over symmetry unique shell pairs |
CSymmSCMatrix | Abstract base class for symmetric double valued matrices |
CSymmSCMatrix2SCExtrapData | |
CSymmSCMatrix4SCExtrapData | |
CSymmSCMatrixdouble | |
CSymmSCMatrixNSCExtrapData | |
CSymmSCMatrixSCExtrapData | |
CSymmSCMatrixSCExtrapError | |
CSymmTwoBodyIntIter | Iterator over symmetry unique shell quartets |
CSymmTwoBodyTwoCenterIntIter | Iterator over symmetry unique shell pairs |
CSymRep | N dimensional matrix representation of a symmetry operation, such as a rotation or reflection |
CSyscallFailed | This is thrown when an system call fails with an errno |
CSystemException | This is thrown when a system problem occurs |
CTaylor_Fjt | Uses Taylor interpolation of up to 8-th order to compute the Boys function |
CTaylorMolecularEnergy | |
CTBGrad | |
CTCHF | Two-determinant wave function for open-shell singlet electronic configurations |
CTCSCF | SCF implementation for open-shell singlet electronic configurations |
CTensor | |
CTensorExtrapData | |
CTensorExtrapError | |
CTensorIndexRangeIterator | TensorIndexRangeIterator is a direct product of shell ranges for each center |
CTestEffH | |
CTestRunnable | |
CThread | The Thread abstract class defines an interface which must be implemented by classes wishing to be run as threads |
Cthreaded_iterator | |
CThreadGrp | The ThreadGrp abstract class provides a means to manage separate threads of control |
CThreadLock | The ThreadLock abstract class provides mutex locks to be used in conjunction with ThreadGrp's |
CThreadLockHolder | Acquire a lock on creation and release it on destruction |
CThreadReplicated | |
CThreadTimer | |
Ctime_accumulator_factory | |
CTimedRegion | TimedRegion is a helper class for RegionTimer |
CTimer | Uses RegionTimer to time intervals in an exception safe manner |
CTimerHolder | |
CToleranceExceeded | This is thrown when when some tolerance is exceeded |
CTorsSimpleCo | Describes an torsion internal coordinate of a molecule |
CTransform | |
CTransformedDensityFitting | Computes density fitting for |ij) density from fitting of |iq) DensityFitting where q is the AO space supporting j |
CTranslateData | Generic data translation |
CTranslateDataByteSwap | Data translation to an external representation with bytes swapped |
CTranslateDataIn | Convert data from other formats |
CTranslateDataOut | Convert data to other formats |
CTriangle | |
CTriangleIntegrator | |
CTriangulatedImplicitSurface | |
CTriangulatedSurface | |
CTriangulatedSurfaceIntegrator | |
CTriInterpCoef | |
CTriInterpCoefKey | |
Ctristate_less | |
CTwoBodyDerivInt | This is an abstract base type for classes that compute geometric derivatives of the integrals involving two electrons and four basis functions |
CTwoBodyDerivIntLibint2 | This implements electron repulsion derivative integrals in the IntV3 library |
CTwoBodyDerivIntV3 | This implements electron repulsion derivative integrals in the IntV3 library |
CTwoBodyFockMatrixBuilder | Builds the two-body part of the Fock matrix in AO basis using integral-direct algorithm |
CTwoBodyFockMatrixDFBuilder | Builds the two-body part of the Fock matrix in AO basis using DF-based algorithm |
CTwoBodyFockMatrixTransformBuilder | Builds the two-body part of the Fock matrix in MO basis using AO->MO transforms |
CTwoBodyGrid | Class TwoBodyGrid describes a set of coordinates of 2 particles |
CTwoBodyInt | This is an abstract base type for classes that compute integrals involving two electrons and 2 functions per electron |
CTwoBodyIntBatch | This is an abstract base type for classes that compute integrals involving two electrons and 2 functions per electron |
CTwoBodyIntBatchGeneric | This is a generic implementation of TwoBodyIntBatch in terms of a TwoBodyInt |
CTwoBodyIntDescrCreator | Creates TwoBodyIntDescr for correlation factor C |
CTwoBodyIntEval | This is an abstract base type for classes that compute integrals involving two electrons and 2 functions per electron |
CTwoBodyIntEvalType | Returns the type of the evaluator for evaluating this set of two-body integrals |
CTwoBodyIntEvalType< 2 > | |
CTwoBodyIntEvalType< 3 > | |
CTwoBodyIntEvalType< 4 > | |
CTwoBodyIntIter | |
CTwoBodyIntLayout | Describes the physical layout of the integrals in TwoBodyIntsAcc |
CTwoBodyIntLibint2 | This implements 4-center two-electron integrals in the IntLibint2 library |
CTwoBodyIntParamsType | Which parameter set needed to specify the operator set? |
CTwoBodyIntParamsType< TwoBodyOperSet::DeltaFunction > | |
CTwoBodyIntParamsType< TwoBodyOperSet::ERI > | |
CTwoBodyIntParamsType< TwoBodyOperSet::G12 > | |
CTwoBodyIntParamsType< TwoBodyOperSet::G12_T1_G12 > | |
CTwoBodyIntParamsType< TwoBodyOperSet::G12DKH > | |
CTwoBodyIntParamsType< TwoBodyOperSet::G12NC > | |
CTwoBodyIntParamsType< TwoBodyOperSet::R12 > | |
CTwoBodyIntParamsType< TwoBodyOperSet::R12_0_G12 > | |
CTwoBodyIntParamsType< TwoBodyOperSet::R12_m1_G12 > | |
CTwoBodyIntShape | Describes types of integrals of 2-body operators |
CTwoBodyIntTraits | Traits of a set of two-body integrals |
CTwoBodyIntType | |
CTwoBodyIntType< 2 > | |
CTwoBodyIntType< 3 > | |
CTwoBodyIntType< 4 > | |
CTwoBodyIntV3 | This implements electron repulsion integrals in the IntV3 library |
CTwoBodyMOIntsRuntime | Smart runtime support for computing MO-basis integrals |
CTwoBodyMOIntsRuntimeUnion23 | TwoBodyMOIntsRuntimeUnion23 packages 2-center and 3-center runtimes; it also keeps track of 2-center matrix inverses |
►CTwoBodyMOIntsTransform | TwoBodyMOIntsTransform computes two-body integrals in MO basis using parallel integrals-direct AO->MO transformation |
CMOSpaces | Predefined enumerated type for the MO spaces |
CTwoBodyMOIntsTransform_123Inds | |
CTwoBodyMOIntsTransform_12Inds | |
CTwoBodyMOIntsTransform_13Inds | |
CTwoBodyMOIntsTransform_ijxy | TwoBodyMOIntsTransform_ijxy computes (ij|xy) integrals using parallel integrals-direct AO->MO transformation |
CTwoBodyMOIntsTransform_ikjy | TwoBodyMOIntsTransform_ikjy computes (ik|jy) integrals using parallel integrals-direct AO->MO transformation |
CTwoBodyMOIntsTransform_iRjS | TwoBodyMOIntsTransform_iRjS computes (iR|jS), or <ij|RS> integrals, where R and S are atomic orbitals, using parallel integral-direct AO->MO transformation |
CTwoBodyMOIntsTransform_ixjy | TwoBodyMOIntsTransform_ixjy computes (ix|jy) integrals using parallel integrals-direct AO->MO transformation |
CTwoBodyMOIntsTransform_ixjy_df | TwoBodyMOIntsTransform_ixjy_df computes (ix|jy) integrals using parallel integral-direct density-fitting |
CTwoBodyNCenterIntDescr | Implements descriptors for various two-body evaluators |
CTwoBodyOper | Describes two-body operators |
CTwoBodyOperDescr | Describes permutational properties (hermiticity, Bose/Fermi) of a two-body operator |
CTwoBodyOperSet | Known two-body operator sets |
CTwoBodyOperSetDescr | Describes sets of two-body operator |
CTwoBodyOperSetProperties | Describes sets of two-body operators ( |
CTwoBodyOperSetProperties< TwoBodyOperSet::DeltaFunction > | |
CTwoBodyOperSetProperties< TwoBodyOperSet::ERI > | |
CTwoBodyOperSetProperties< TwoBodyOperSet::G12 > | |
CTwoBodyOperSetProperties< TwoBodyOperSet::G12_T1_G12 > | |
CTwoBodyOperSetProperties< TwoBodyOperSet::G12DKH > | |
CTwoBodyOperSetProperties< TwoBodyOperSet::G12NC > | |
CTwoBodyOperSetProperties< TwoBodyOperSet::R12 > | |
CTwoBodyOperSetProperties< TwoBodyOperSet::R12_0_G12 > | |
CTwoBodyOperSetProperties< TwoBodyOperSet::R12_m1_G12 > | |
CTwoBodySODerivInt | TwoBodySODerivInt computes four-center two-electron derivative integrals in a symmetry-adapted basis |
CTwoBodySOInt | TwoBodySOInt computes four-center two-electron integrals in a symmetry-adapted basis |
CTwoBodyTensorInfo | Provides information about the type of a two body tensor |
CTwoBodyThreeCenterDerivInt | This is an abstract base type for classes that compute three centers integrals involving two electrons |
CTwoBodyThreeCenterInt | This is an abstract base type for classes that compute integrals involving two electrons in three Gaussian functions |
CTwoBodyThreeCenterIntLibint2 | This implements 3-center 2-body integrals in the IntLibint2 library |
CTwoBodyThreeCenterIntV3 | This implements electron repulsion integrals involving three centers in the IntV3 library |
CTwoBodyThreeCenterMOIntsTransform | TwoBodyThreeCenterMOIntsTransform computes (xy|z) integrals, using parallel integral-direct AO->MO transformation |
CTwoBodyThreeCenterMOIntsTransform_ijR | TwoBodyThreeCenterMOIntsTransform_ijR computes (ij|R) integrals, where R are atomic orbitals, using parallel integral-direct AO->MO transformation |
CTwoBodyThreeCenterMOIntsTransform_ijR_using_iqR | TwoBodyThreeCenterMOIntsTransform_ijR computes (ij|R) integrals, where R are atomic orbitals, using (iq|R) integrals |
CTwoBodyTwoCenterDerivInt | This is an abstract base type for classes that compute two centers integrals involving two electrons |
CTwoBodyTwoCenterInt | This is an abstract base type for classes that compute integrals involving two electrons in two Gaussian functions |
CTwoBodyTwoCenterIntIter | |
CTwoBodyTwoCenterIntLibint2 | This implements 2-center 2-body integrals in the IntLibint2 library |
CTwoBodyTwoCenterIntOp | The 2-body analog of OneBodyIntOp |
CTwoBodyTwoCenterIntV3 | This implements electron repulsion integrals involving two centers in the IntV3 library |
Ctype_info_key | |
CUHF | This provides an unrestricted Hartree-Fock implementation |
CUKS | This provides a Kohn-Sham implementation for unrestricted-orbital open-shell systems |
CUncapped5SphereExclusionShape | |
CUncappedTorusHoleShape | |
CUncontractedBasisSet | Used to form uncontracted Gaussian basis sets |
CUnionBasisSet | UnionBasisSet constructs a union of two GaussianBasisSet objects |
CUnionShape | A UnionShape is volume enclosed by a set of Shape's |
CUnits | Used to perform unit conversions |
CUnrestrictedSCF | A base class for unrestricted self-consistent-field methods |
CUsedData | |
CVDWShape | Describes the surface of a molecule as the union of atom centered spheres, each the van der Waals radius of the atom |
Cvec2 | |
Cvec3 | |
Cvec4 | |
CVertex | |
CVolume | A Volume is a Function of three variables |
CVWN1LCFunctional | The VWN1LCFunctional computes energies and densities using the VWN1 local correlation term (from Vosko, Wilk, and Nusair) |
CVWN2LCFunctional | The VWN2LCFunctional computes energies and densities using the VWN2 local correlation term (from Vosko, Wilk, and Nusair) |
CVWN3LCFunctional | The VWN3LCFunctional computes energies and densities using the VWN3 local correlation term (from Vosko, Wilk, and Nusair) |
CVWN4LCFunctional | The VWN4LCFunctional computes energies and densities using the VWN4 local correlation term (from Vosko, Wilk, and Nusair) |
CVWN5LCFunctional | The VWN5LCFunctional computes energies and densities using the VWN5 local correlation term (from Vosko, Wilk, and Nusair) |
CVWNLCFunctional | An abstract base class from which the various VWN (Vosko, Wilk and Nusair) local correlation functional (1, 2, 3, 4, 5) classes are derived |
CWavefunction | A Wavefunction is a MolecularEnergy that utilizies a GaussianBasisSet |
CWavefunctionWorld | Class WavefunctionWorld describes the environment of a Wavefunction |
CWriteBasisGrid | |
CWriteElectronDensity | Writes the electron density at user defined grid points to the standard output or to a separate file |
CWriteElectrostaticPotential | Writes the electrostatic potential at user defined grid points to the standard output or to a separate file |
CWriteGrid | The abstract WriteGrid class provides an interface for writing the value of a scalar function evaluated at a given set of grid points to a file |
CWriteMolden | |
CWriteOrbital | Writes an orbital at user defined grid points to the standard output or to a separate file |
CWriteOrbitals | Writes orbitals at user defined grid points to the standard output or to a separate file |
►CWriteVectorGrid | WriteVectorGrid provides an interface for writing the value of a vector function evaluated at a given set of grid points to a file (compare to WriteGrid) |
CDimensionMap | |
CX | |
CXalphaFunctional | Implements the Xalpha exchange functional |
CXMLDataStream | |
CXMLDataStreamTranslator | |
CXMLReadable | |
CXMLReader | |
CXMLWritable | |
CXMLWriter | |
CY | |
►Nstd | STL namespace |
Chash< sc::FermionOccupationBlockString > | Specialization of std::hash for sc::FermionOccupationBlockString |
Chash< sc::FermionOccupationDBitString > | Specialization of std::hash for sc::FermionOccupationDBitString |
Chash< sc::FermionOccupationNBitString< Ns > > | Specialization of std::hash for sc::FermionOccupationNBitString |
►NTiledArray | |
►Nexpressions | |
CTensorExpression | |
Cfunction_iterable | |
CGlobalFixture | |
CIterableBasisElementData | |
CIterableBasisElementData< Iterator, ShellBlockIterator< Iterable > > | |
Cshell_block_iterable | |
Cshell_iterable | |
►CShellBlockIterator | |
CSkeleton | |
CShellData | |