ARTS
2.4.0(git:4fb77825)
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Wigner symbol interactions. More...
Go to the source code of this file.
Classes | |
struct | Wigner3JTriangleLimit |
Macros | |
#define | WIGNER3 wig3jj |
#define | WIGNER6 wig6jj |
Functions | |
Numeric | wigner3j (const Rational j1, const Rational j2, const Rational j3, const Rational m1, const Rational m2, const Rational m3) |
Wigner 3J symbol. More... | |
Numeric | wigner6j (const Rational j1, const Rational j2, const Rational j3, const Rational l1, const Rational l2, const Rational l3) |
Wigner 6J symbol. More... | |
Numeric | co2_ecs_wigner_symbol (int Ji, int Jf, int Ji_p, int Jf_p, int L, int li, int lf) |
Returns the wigner symbol used in Niro etal 2004. More... | |
Numeric | o2_ecs_wigner_symbol (int Nl, int Nk, int Jl, int Jk, int Jl_p, int Jk_p, int L) |
Returns the wigner symbol used in Makarov etal 2013. More... | |
constexpr Wigner3JTriangleLimit | find_wigner3j_limits (const Rational L1, const Rational L2) |
Finds the upper and lower limits of L3 given a Wigner-3J symbol: More... | |
constexpr Wigner3JTriangleLimit | find_even_limits (const Wigner3JTriangleLimit lim1, const Wigner3JTriangleLimit lim2) |
Combines two limits and return the highest even-numbered low value and the lowest numbered even high value. More... | |
Numeric | o2_ecs_erot_jn_same (Rational J) |
Energy of the J=N line at J. More... | |
Numeric | o2_ecs_ql_makarov (Rational L, Numeric T) |
Numeric | o2_ecs_adiabatic_factor_makarov (Rational N, Numeric T) |
Numeric | o2_ecs_wigner_symbol_tran (const Rational &Ji, const Rational &Jf, const Rational &Ni, const Rational &Nf, const Rational &Si, const Rational &Sf, const Rational &Ji_p, const Rational &Jf_p, const Rational &Ni_p, const Rational &Nf_p, const Rational &n, const Numeric &T) |
Returns the wigner symbol used in Tran etal 2006. More... | |
Numeric | o2_makarov2013_reduced_dipole (const Rational &Jup, const Rational &Jlo, const Rational &N) |
Returns the reduced dipole moment following Makarov etal 2013. More... | |
Index | make_wigner_ready (int largest, [[maybe_unused]] int fastest, int size) |
bool | is_wigner_ready (int j) |
Tells if the function can deal with the input integer. More... | |
bool | is_wigner3_ready (const Rational &J) |
Tells if the function is ready for Wigner 3J calculations. More... | |
bool | is_wigner6_ready (const Rational &J) |
Tells if the function is ready for Wigner 6J calculations. More... | |
#define WIGNER3 wig3jj |
Definition at line 36 of file wigner_functions.cc.
#define WIGNER6 wig6jj |
Definition at line 37 of file wigner_functions.cc.
Numeric co2_ecs_wigner_symbol | ( | int | Ji, |
int | Jf, | ||
int | Ji_p, | ||
int | Jf_p, | ||
int | L, | ||
int | li, | ||
int | lf | ||
) |
Returns the wigner symbol used in Niro etal 2004.
Symbol: / \ / \ / \ | Ji_p L Ji | | Jf_p L Jf | | Ji Jf 1 | | | | | < > (2L + 1) | li 0 -li | | -lf 0 lf | | Jf_p Ji_p L | \ / \ / \ /
Note: The wigner library takes two times the physical values so, e.g., the 1 must be 2. This hold true for all user inputs as well!
Reference: Spectra calculations in central and wing regions of CO2 IR bands between 10 and 20 mcrons. I: model and laboratory measurements. F. Niro, C. Boulet, J.-M. Hartmann. JQSRT 88 (2004) 483 – 498. Equation 4 page 488.
Note: Ignore typos, the above is tested in relmat
Warning: Must have called wig_temp_init(j) with appropriate j before using this function. Failure to do so will cause segfault.
[in] | Ji | as above times 2 |
[in] | Jf | as above times 2 |
[in] | Ji_p | as above times 2 |
[in] | Jf_p | as above times 2 |
[in] | L | as above times 2 |
[in] | li | as above times 2 |
[in] | lf | as above times 2 |
Definition at line 88 of file wigner_functions.cc.
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constexpr |
Combines two limits and return the highest even-numbered low value and the lowest numbered even high value.
[in] | lim1 | Limit 1 |
[in] | lim2 | Limit 2 |
Definition at line 136 of file wigner_functions.cc.
References Wigner3JTriangleLimit::lower, and Wigner3JTriangleLimit::upper.
Referenced by o2_ecs_wigner_symbol_tran().
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constexpr |
Finds the upper and lower limits of L3 given a Wigner-3J symbol:
/ \
L1 L2 L3 |
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M1 M2 M3 |
\ /
Based on abs(L1-L2) <= L3 <= L1+L2, where L1 and L2 are positives
[in] | L1 | As in Wigner symbol |
[in] | L2 | As in Wigner symbol |
Definition at line 122 of file wigner_functions.cc.
References abs.
Referenced by o2_ecs_wigner_symbol_tran().
bool is_wigner3_ready | ( | const Rational & | J | ) |
Tells if the function is ready for Wigner 3J calculations.
[in] | J | Largest input into a Wigner 3J function call |
Definition at line 319 of file wigner_functions.cc.
References is_wigner_ready(), and Rational::toInt().
bool is_wigner6_ready | ( | const Rational & | J | ) |
Tells if the function is ready for Wigner 6J calculations.
[in] | J | Largest input into a Wigner 6J function call |
Definition at line 325 of file wigner_functions.cc.
References is_wigner_ready(), and Rational::toInt().
bool is_wigner_ready | ( | int | j | ) |
Tells if the function can deal with the input integer.
[in] | j |
Definition at line 313 of file wigner_functions.cc.
Referenced by is_wigner3_ready(), and is_wigner6_ready().
Index make_wigner_ready | ( | int | largest, |
[[maybe_unused] ] int | fastest, | ||
int | size | ||
) |
Definition at line 276 of file wigner_functions.cc.
Referenced by test_ecs20(), test_hitran2017(), Wigner3Init(), and Wigner6Init().
Definition at line 196 of file wigner_functions.cc.
References Conversion::angstrom2meter(), N, o2_ecs_erot_jn_same(), and Constant::pow2().
Referenced by o2_ecs_wigner_symbol_tran().
Energy of the J=N line at J.
[in] | J | Rotational quantum number |
Definition at line 159 of file wigner_functions.cc.
References Constant::pow2(), and Constant::pow3().
Referenced by o2_ecs_adiabatic_factor_makarov(), and o2_ecs_ql_makarov().
Definition at line 183 of file wigner_functions.cc.
References beta, o2_ecs_erot_jn_same(), and pow().
Referenced by o2_ecs_wigner_symbol_tran().
Numeric o2_ecs_wigner_symbol | ( | int | Nl, |
int | Nk, | ||
int | Jl, | ||
int | Jk, | ||
int | Jl_p, | ||
int | Jk_p, | ||
int | L | ||
) |
Returns the wigner symbol used in Makarov etal 2013.
Symbol: / \ / \ / \ / \ | Nl Nk L | | L Jk Jl | | L Jk_p Jl_p | | L Jk Jl | | | < > < > < > | 0 0 0 | | 1 Nl Nk | | 1 Nl Nk | | 1 Jl_p Jk_p | \ / \ / \ / \ /
Note: The wigner library takes two times the physical values so, e.g., the 1 must be 2. This hold true for all user inputs as well!
Reference: D.S. Makarov, M.Yu. Tretyakov, C. Boulet, Line mixing in the 60-GHz atmospheric oxygen band: Comparison of the MPM and ECS model, Journal of Quantitative Spectroscopy and Radiative Transfer, Volume 124, 2013, Pages 1-10, ISSN 0022-4073, https://doi.org/10.1016/j.jqsrt.2013.02.019. (http://www.sciencedirect.com/science/article/pii/S0022407313000745) Abstract: Precise profiles of the 60-GHz molecular oxygen band recorded earlier in a wide temperature range by means of a resonator spectrometer at atmospheric pressure were treated. High signal-to-noise ratio allows careful study of the band shape taking into consideration the mixing effect. Comparative analysis of the band profile calculated by an extended MPM (Millimeter-wave Propagation Model) and by the ECS (Energy Corrected Sudden) approximation model is presented. Some limitations of the MPM approach are discussed on the basis of the comparison of the two models. Interbranch coupling is shown to make a noticeable contribution to absorption which means that it should be taken into account as it is expected to improve band profile modeling accuracy. Keywords: Molecular oxygen; Microwave spectroscopy; Profile shape modeling; Collisional coupling
Note: The ARTS implementation has not been tested in detail
Warning: Must have called wig_temp_init(j) with appropriate j before using this function. Failure to do so will cause segfault.
[in] | Nl | as above times 2 |
[in] | Nk | as above times 2 |
[in] | Jl | as above times 2 |
[in] | Jk | as above times 2 |
[in] | Jl_p | as above times 2 |
[in] | Jk_p | as above times 2 |
[in] | L | as above times 2 |
Definition at line 94 of file wigner_functions.cc.
Numeric o2_ecs_wigner_symbol_tran | ( | const Rational & | Ji, |
const Rational & | Jf, | ||
const Rational & | Ni, | ||
const Rational & | Nf, | ||
const Rational & | Si, | ||
const Rational & | Sf, | ||
const Rational & | Ji_p, | ||
const Rational & | Jf_p, | ||
const Rational & | Ni_p, | ||
const Rational & | Nf_p, | ||
const Rational & | n, | ||
const Numeric & | T | ||
) |
Returns the wigner symbol used in Tran etal 2006.
Symbol: / \ / \ / \ / \ / \ | Ni_p Ni L | | Nf_p Nf L | | L Ji Ji_p | | L Jf Jf_p | | L Ji Ji_p | | | | | < > < > < > (2L + 1) (OmegaNi / OmegaL) * QL | 0 0 0 | | 0 0 0 | | Si Ni_p Ni | < Sf Nf_p Nf | | n Jf_p Jf | \ / \ / \ / \ / \ /
Reference: H. Tran, C. Boulet, and J.-M. Hartmann Line mixing and collision-induced absorption by oxygen in the A band: Laboratory mea*surements, model, and tools for atmospheric spectra computations, Journal Of Geophysical Research, Volume 111, 2006, doi:10.1029/2005JD006869.
Note: The ARTS implementation has not been tested in detail
Warning: Must have called wig_temp_init(j) with appropriate j before using this function. Failure to do so will cause segfault.
[in] | Ji | Initial J of level |
[in] | Jf | Final J of level |
[in] | Ni | Initial N of level |
[in] | Nf | Final N of level |
[in] | Si | Initial S of level |
[in] | Sf | Final S of level |
[in] | Ji_p | Initial J of pseudo-level |
[in] | Jf_p | Final J of pseudo-level |
[in] | Ni_p | Initial N of pseudo-level |
[in] | Nf_p | Final N of pseudo-level |
[in] | L | Coupling to pseudo-level |
[in] | n | Order of the tensor (n=1 is magnetic dipole) |
[in] | OmegaNi | Adiabatic factor at initial N |
[in] | OmegaL | Adiabatic factor at L |
[in] | QL | Adiabatic factor at L |
Definition at line 218 of file wigner_functions.cc.
References even(), find_even_limits(), find_wigner3j_limits(), max, o2_ecs_adiabatic_factor_makarov(), o2_ecs_ql_makarov(), o2_ecs_wigner_symbol_tran(), sqrt(), Rational::toInt(), and WIGNER3.
Referenced by o2_ecs_wigner_symbol_tran().
Numeric o2_makarov2013_reduced_dipole | ( | const Rational & | Jup, |
const Rational & | Jlo, | ||
const Rational & | N | ||
) |
Returns the reduced dipole moment following Makarov etal 2013.
Only for N+ and N- lines
[in] | Jup | Upper state's J |
[in] | Jlo | Lower state's J |
[in] | N | Upp/low states' N |
Definition at line 267 of file wigner_functions.cc.
References even(), N, sqrt(), Rational::toInt(), and WIGNER6.
Numeric wigner3j | ( | const Rational | j1, |
const Rational | j2, | ||
const Rational | j3, | ||
const Rational | m1, | ||
const Rational | m2, | ||
const Rational | m3 | ||
) |
Wigner 3J symbol.
Run wigxjpf wig3jj for Rational symbol
/ \
j1 j2 j3 |
---|
m1 m2 m3 |
\ /
See for definition: http://dlmf.nist.gov/34.2
[in] | j1 | as above |
[in] | j2 | as above |
[in] | j3 | as above |
[in] | m1 | as above |
[in] | m2 | as above |
[in] | m3 | as above |
Definition at line 40 of file wigner_functions.cc.
Referenced by Zeeman::Model::Strength().
Numeric wigner6j | ( | const Rational | j1, |
const Rational | j2, | ||
const Rational | j3, | ||
const Rational | l1, | ||
const Rational | l2, | ||
const Rational | l3 | ||
) |
Wigner 6J symbol.
Run wigxjpf wig6jj for Rational symbol
/ \ | j1 j2 j3 | < > | l1 l2 l3 | \ /
See for definition: http://dlmf.nist.gov/34.4
[in] | j1 | as above |
[in] | j2 | as above |
[in] | j3 | as above |
[in] | l1 | as above |
[in] | l2 | as above |
[in] | l3 | as above |
Definition at line 65 of file wigner_functions.cc.
Referenced by Absorption::reduced_magnetic_quadrapole().