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ampsci
High-precision calculations for one- and two-valence atomic systems
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Low qr form of Pseudoscalar multipole operator: \( P_K = S^5_K = t^K(q)(i\gamma^0\gamma^5)\) NOTE: If K=0, omega should be (ea-eb); for K=1 should be q = alpha*omega!
#include <EM_multipole_lowqr.hpp>
Inheritance diagram for DiracOperator::S5k_lowq:Public Member Functions | |
| S5k_lowq (const Grid &gr, int K, double omega, double alpha=PhysConst::alpha) | |
| DiracSpinor | radial_rhs (const int kappa_a, const DiracSpinor &Fb) const override final |
| Computes the right-hand spinor dF_b for the radial integral. | |
| double | radialIntegral (const DiracSpinor &Fa, const DiracSpinor &Fb) const override final |
| Radial integral R_ab, defined by RME = angularF(a,b) * radialIntegral(a,b). | |
| void | updateFrequency (const double omega) override final |
| NOTE: If K=0, omega should be (ea-eb); for K=1 should be q = alpha*omega! | |
Public Member Functions inherited from DiracOperator::EM_multipole | |
| const SphericalBessel::JL_table * | jl () const |
| Returns the precomputed Bessel table pointer (may be nullptr). | |
| std::string | name () const override |
| Returns a human-readable label, e.g. "T^E_1", "T^M5_2", "t_1", "P_1". | |
| double | angularF (const int ka, const int kb) const override |
| Angular factor linking the radial integral to the reduced matrix element: \( \langle a \| h \| b \rangle = F(\kappa_a,\kappa_b) \cdot
\int \! dr \). | |
| void | updateRank (int new_K) override |
| Updates the tensor rank and adjusts parity accordingly. | |
| std::unique_ptr< TensorOperator > | clone () const override |
| Creates a fully independent copy of this operator at its current (rank, frequency) state via the MultipoleOperator factory. | |
| EM_multipole (const EM_multipole &)=default | |
| EM_multipole & | operator= (const EM_multipole &)=default |
| EM_multipole (EM_multipole &&)=default | |
| EM_multipole & | operator= (EM_multipole &&)=default |
Public Member Functions inherited from DiracOperator::TensorOperator | |
| TensorOperator (const TensorOperator &)=default | |
| TensorOperator & | operator= (const TensorOperator &)=default |
| TensorOperator (TensorOperator &&)=default | |
| TensorOperator & | operator= (TensorOperator &&)=default |
| bool | freqDependantQ () const |
| Returns true if the operator is frequency-dependent (requires updateFrequency() calls). | |
| bool | isZero (int ka, int kb) const |
| Returns true if <a|h|b> = 0 by rank/parity selection rules. | |
| bool | isZero (const DiracSpinor &Fa, const DiracSpinor &Fb) const |
| Overload taking DiracSpinors; forwards to isZero(ka, kb). | |
| bool | selectrion_rule (int twoJA, int piA, int twoJB, int piB) const |
| Returns true if the matrix element is non-zero by angular momentum and parity selection rules (arguments are 2j and pi as integers). | |
| const std::vector< double > & | getv () const |
| Returns a const ref to the stored vector v. | |
| double | getc () const |
| Returns the "overall" constant c. | |
| bool | imaginaryQ () const |
| returns true if operator is imaginary (has imag MEs) | |
| int | rank () const |
| Rank k of operator. | |
| int | parity () const |
| returns parity, as integer (+1 or -1) | |
| int | symm_sign (const DiracSpinor &Fa, const DiracSpinor &Fb) const |
| returns relative sign between <a||x||b> and <b||x||a> | |
| virtual std::string | units () const |
| Returns units of operator as a string (usually au, may be MHz, etc.) | |
| virtual double | angularCff (int kappa_a, int kappa_b) const |
| Angular coefficient C_ff for the f_a*f_b term of the radial integral. | |
| virtual double | angularCgg (int, int) const |
| Angular coefficient C_gg for the g_a*g_b term of the radial integral. | |
| virtual double | angularCfg (int, int) const |
| Angular coefficient C_fg for the f_a*g_b term of the radial integral. | |
| virtual double | angularCgf (int, int) const |
| Angular coefficient C_gf for the g_a*f_b term of the radial integral. | |
| double | angularCxy (uint8_t x, uint8_t y, int kappa_a, int kappa_b) const |
| Dispatches to angularCff/fg/gf/gg based on component indices x, y. | |
| double | rme3js (int twoja, int twojb, int two_mb=1, int two_q=0) const |
| 3j-symbol factor linking the full ME to the RME. | |
| double | rme3js (const DiracSpinor &Fa, const DiracSpinor &Fb, int two_mb=1, int two_q=0) const |
| Overload of rme3js taking DiracSpinors. | |
| DiracSpinor | reduced_rhs (const int ka, const DiracSpinor &Fb) const |
| Returns angularF(ka,kb) * radial_rhs(ka,Fb); spinor-valued RME action on Fb, used in perturbation theory/TDHF. | |
| DiracSpinor | reduced_lhs (const int ka, const DiracSpinor &Fb) const |
| As reduced_rhs but for the conjugate direction; Fb * reduced_lhs(ka, Fb) = <b||h||a>. | |
| double | reducedME (const DiracSpinor &Fa, const DiracSpinor &Fb) const |
| Returns the reduced matrix element <a||h||b> = A_ab * R_ab. | |
| double | fullME (const DiracSpinor &Fa, const DiracSpinor &Fb, std::optional< int > two_ma=std::nullopt, std::optional< int > two_mb=std::nullopt, std::optional< int > two_q=std::nullopt) const |
| Returns "full" matrix element, for optional (ma, mb, q) [taken as int 2*]. If not specified, returns z-component (q=0), with ma=mb=min(ja,jb) | |
| double | matel_factor (MatrixElementType type, int twoJa, int twoJb) const |
| Returns the factor to convert a reduced ME to a different form (Reduced, Stretched, or HFConstant); see MatrixElementType. | |
| double | matel_factor (MatrixElementType type, const DiracSpinor &Fa, const DiracSpinor &Fb) const |
| Overload of matel_factor taking DiracSpinors. | |
Additional Inherited Members | |
Protected Member Functions inherited from DiracOperator::EM_multipole | |
| EM_multipole (int rank_k, Parity pi, double constant, const std::vector< double > &vec, Realness RorI, bool freq_dep, const Grid *grid, char type, char comp, bool low_q, const SphericalBessel::JL_table *jl=nullptr, char form='V') | |
| Initialise the EM_multipole base layer. | |
Protected Member Functions inherited from DiracOperator::TensorOperator | |
| TensorOperator (int rank_k, Parity pi, double constant=1.0, const std::vector< double > &vec={}, Realness RorI=Realness::real, bool freq_dep=false) | |
| Constructs a specific tensor operator. Called by derived classes. | |
Protected Attributes inherited from DiracOperator::EM_multipole | |
| const Grid * | m_grid {nullptr} |
| double | m_omega |
| Current frequency; cached by each derived updateFrequency(). | |
| char | m_type {} |
| char | m_comp {} |
| bool | m_low_q {} |
| char | m_form {} |
| const SphericalBessel::JL_table * | m_jl {nullptr} |
Protected Attributes inherited from DiracOperator::TensorOperator | |
| int | m_rank |
| Parity | m_parity |
| Realness | m_Realness |
| bool | m_freqDependantQ {false} |
| double | m_constant |
| std::vector< double > | m_vec |
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inlinefinaloverridevirtual |
Computes the right-hand spinor dF_b for the radial integral.
Returns \( \delta F_b \) such that the radial integral satisfies:
\[ R_{ab} = F_a \cdot \delta F_b = \int_0^\infty \left(f_a\,\delta f_b + g_a\,\delta g_b\right)\,{\rm d}r \]
The default implementation constructs \( \delta F_b \) using the stored radial function \( v(r) \) and the angular coefficients:
\[ \delta F_b(r) = c\,v(r) \begin{pmatrix} C_{ff}\,f_b(r) + C_{fg}\,g_b(r) \\ C_{gf}\,f_b(r) + C_{gg}\,g_b(r) \end{pmatrix} \]
This is used by reduced_rhs() to build \( \langle a \| \hat{h} \| b \rangle \) as a spinor-valued quantity, enabling perturbation theory and TDHF. Override this for operators whose radial structure cannot be expressed in this standard form.
| kappa_a | Relativistic quantum number \( \kappa_a \) of the bra state (needed to evaluate the angular coefficients). |
| Fb | Ket DiracSpinor \( F_b \) . |
Reimplemented from DiracOperator::TensorOperator.
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inlinefinaloverridevirtual |
Radial integral R_ab, defined by RME = angularF(a,b) * radialIntegral(a,b).
Returns the radial part \( R_{ab} \) of the reduced matrix element:
\[ \langle a \| \hat{h} \| b \rangle = A_{ab} \cdot R_{ab} \]
where \( A_{ab} \) is angularF().
The default implementation evaluates \( R_{ab} = F_a \cdot \delta F_b \) , using the default radial structure:
\[ R_{ab} = c\int_0^\infty v(r)\left( C_{ff}\,f_a f_b + C_{fg}\,f_a g_b + C_{gf}\,g_a f_b + C_{gg}\,g_a g_b \right)\,{\rm d}r \]
Override this for operators that do not fit this standard form. If radial_rhs() is also overridden, both must remain mutually consistent.
Reimplemented from DiracOperator::TensorOperator.
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inlinefinaloverridevirtual |
NOTE: If K=0, omega should be (ea-eb); for K=1 should be q = alpha*omega!
Reimplemented from DiracOperator::TensorOperator.