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| = TD-DFT/SOC = SOC计算的输入文件中以$section name ... $end符号为划分分为6段: |
##master-page:HelpTemplate ##master-date:Unknown-Date #format wiki #language en #Please change following line to BDF module name |
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| . $compass 为基组和坐标控制（如果要计算其他化合物，选用其他基组，可修改这一段）； $xuanyuan 为积分控制，基本不需要改动，除非需要使用cam-b3lyp这段要加入两行：RS和0.33d0，控制计算新的积分; $scf为计算方法控制，可选用不同泛函； $tddft isf=0 ... 这一段(isf=0)表示计算singlet $tddft isf=1 ... 计算triplet $tddft isoc=2 ...根据前面两个计算的结果来计算soc state interaction，imatsoc为控制打印旋轨耦合矩阵元，格式如下： IMATSOC n fileA symA stateA fileB symB stateB fileA' symA' stateA' fileB' symB' stateB' . .. . .. n代表要打印几个态的旋轨耦合矩阵元<A|hso|B>，接着后面为要打印矩阵元两个态的描述，每个态由(file,sym,state)3个量表示，file表示前面第几个tddft的文件，sym表示该计算中第几个不可约表示，state表示该不可约表示里的第几个态。如输入文件中（0，0，0，2，1，1）表示基态和file2即triplet，sym＝1的第一个态(即T1)，之间的旋轨耦合矩阵元。 = Example = |
= tddft: time-dependent density functional theory = <<TableOfContents(4)>> |
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| Time dependent DFT/HF calculation. Support Full TDDFT, TDA and RPA. }}} == Quick guides == The following examples give the minimal inputs for starting TD-DFT calculations. |
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| $COMPASS Title | 1. [[Closed-shell Systems : R-TD-DFT]] |
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| . ir1 | 2. [[Open-shell Systems : U-TD-DFT and spin-adapted TD-DFT for spin-conserving excitations]] |
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| Basis | 3. [[Open-shell Systems : Spin-flip TD-DFT for spin-flip excitations]] |
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| . IRCOMPLEX | 4. [[TD-DFT with SOC]] |
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| Geometry | == General keywords == === imethod === === isf === === itda === === idrpa === === ispa === === ialda === === thrdab === === itest === === icorrect === === itrans === === iro === === icv === === ioo === === iksf === === iact === === elw === === eup === === idiag === === ndiag === === aokxc === |
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| . Ir -0.0117154745 0.02136826 -0.1871622466 C -1.590674169 0.7736105591 0.850482009 C -4.0103593084 1.6631710744 2.0881698872 C -1.587030516 1.6064254297 1.9846531563 C -2.8754743453 0.4162567381 0.3762778017 C -4.0684588604 0.8406678872 0.9653728357 C -2.7652566303 2.0433988261 2.5945234724 H -0.633533598 1.9127046365 2.4024890794 H -5.031807216 0.5389051931 0.5644872718 H -2.7118027246 2.6839610147 3.4712663621 H -4.9285536031 2.0014173162 2.5588819363 C 1.4053272337 1.0109349589 0.8613594531 C 3.3836289249 2.6234305864 2.1354680771 C 2.0771460677 0.5800974992 2.0211645669 C 1.7631262545 2.2970140474 0.3585152663 C 2.7411852479 3.0844966855 0.9939992732 C 3.044957901 1.3650101996 2.6469305081 H 1.8305785647 -0.3881315485 2.4444240781 H 3.0042061929 4.0630294704 0.6010854425 H 3.5407187868 0.9959817385 3.5420383099 H 4.1379887938 3.2338708527 2.6233130653 C 0.1111675725 -1.7119838156 0.8795182027 C 0.5294631611 -4.2465845213 2.136544371 C 1.0417183334 -2.6652412426 0.4024936912 C -0.6004107662 -2.1019903883 2.028797446 C -0.4006210626 -3.3384592866 2.6477946425 C 1.2608503358 -3.9079720636 1.0002003463 H -1.3244348019 -1.413608967 2.4531282601 H -0.9731808696 -3.5946754614 3.5357463104 H 1.9890357565 -4.6057356294 0.596753782 H 0.6876544671 -5.2085686031 2.6147222734 N -1.7055918832 -0.7893527004 -1.3058124454 C -1.9722242221 -1.5767164653 -2.3518797181 C -3.3612772292 -1.7339951323 -2.5010242321 C -3.9194938069 -0.9920736156 -1.4729787184 N -2.8999954385 -0.434228237 -0.7703095731 N 1.5150714233 -1.0583114657 -1.2825131804 C 2.3138081406 -0.9142123699 -2.3433358371 C 3.1082799478 -2.0614459074 -2.5127910698 C 2.7399679653 -2.9098550697 -1.4816601802 N 1.779892419 -2.2802990117 -0.7566347846 H -1.1601491745 -1.9907288667 -2.9313421992 H 3.089224611 -3.8952971699 -1.2184247348 H 3.8501674705 -2.2464169166 -3.2743336863 H -3.8863865729 -2.3105313491 -3.2470045506 H -4.9492341453 -0.8290099882 -1.1983109053 H 2.2814545468 -0.0015798294 -2.9198044757 C 0.5167706643 4.2876200227 -2.6332627231 C -0.4153270812 3.3663568698 -3.1195481682 C -0.5686406908 2.1688169354 -2.4341135463 N 0.1409383672 1.8631654694 -1.3352631181 C 1.05542065 2.7471949823 -0.8428699526 C 1.2493629941 3.9769776219 -1.4963443658 H 0.6676353447 5.2385692731 -3.1359337322 H -1.011339893 3.5685529446 -4.0026032407 H -1.276466123 1.413706092 -2.7596936709 H 1.9731120675 4.6831024371 -1.1074561222 | == Convergence threshold == === crit_e === === crit_vec === |
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| End geometry GROUP C(1) Skeleton $END | == States specification == === iext === === next === == Save eigenvectors == === istore === Integer: specify the file no. to store TDDFT information |
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| $XUANYUAN scalar heff 3 soint hsoc 2 Direct Schwarz $END | === lefteig === By default, in TD-DFT the left eigenvector X-Y is also stored. |
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| $SCF RKS DFT functional | == output eigenvector control == === nprt === === cthrd === == TD-DFT/SOC and Property evaluation == === nfiles === No. of TD-DFT calculations to be loaded. |
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| . B3lyp | === isoc === =1, Only work for closed-shell case (NOT recommended!) |
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| =2, General SOC state interaction =3, just print SOC matrix elements between two spin-free states (without diagonalization Hsoc). === ifgs === =0, default for not including ground state (GS) in SOC treatment; =1, include GS. === imatsoc === Define SOC matrices need to be calculated. Input format looks like {{{ ... #SCF calculation for the ground state S0. It is a singlet. $scf spin 0 ... $end #First TDDFT, singlets S0-S9. $tddft imethod 1 isf 0 iext 10 .... $end #Second TDDFT, triplet T1-T10 $tddft imethod 1 isf 1 iext 10 $end $tddft .... imatsoc 7 0 0 0 2 1 1 0 0 0 2 1 2 1 1 1 2 1 1 1 1 1 2 1 2 1 1 2 2 1 1 1 1 2 2 1 2 2 1 1 2 1 1 2 1 1 2 1 2 $end }}} In this input, 7 means seven of SOC matrices will be calculate '''(If the number <0, then ALL possible HSOC mat will be printed !). '''Here, it is very tricky to specify states: * The string "0 0 0" always treat as the ground state. * For other states, three numbers "n m n" represent "ith-tddft", "symmetry" and "ithstate" respectively. Therefore, the first matrix element "0 0 0 2 1 1" means SOC matrix of <S0|HSOC|T1>. The third matrix element "1 1 1 2 1 1" means SOC matrix <S1|HSOC|T1>. Here, the first "1" in bra state "1 1 1" means the state from first TDDFT calculation. The second and third "1" in the bra state "1 1 1" means this state has spatial symmetry "1" and is the first excited state. === imatrsf === Transition dipole between Spin-free states. The input is similar to '''imatsoc''' (but currently selected printing is not implemented). Simply use -1 to print all of them. === imatrso === Define transition dipole moment need to be printed between two SOC-included states. Input format looks like(notice we omit other input in TDDFT module) {{{ $TDDFT ... imatrso 5 1 1 1 2 1 3 1 4 1 5 ... |
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| }}} Then, "imatrso" is specified to define transition dipole moments need to be printed. The number "5" require transition dipoles between 5-pairs of states to be print. The following 5 lines define which pairs will be printed. Here, we require transition dipoles between the first state and five states are printed. |
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| $TDDFT IMETHOD | === idiag === By default, idiag=0 uses full diagonalization (preferred for small model space). |
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| . 1 | If idiag=1, then TD-DFT/SOC can use Davidson's algorithm also, along with a specification for the no. of states by '''iexit'''. |
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| ISF | === iact === =1, allows to use active space specification for the projected active-orbital SOC Hamiltonian (P*HSOC*P), '''eup''' can be specified in (eV) to give a cut off to define active physically interested excited states. |
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| . 0 ITDA . 0 IDIAG . 1 istore . 1 iexit 10 AOKXC MemJKOP . 2048 crit_e 1.d-4 $END $TDDFT IMETHOD . 1 ISF . 1 ITDA . 0 IDIAG . 1 istore . 2 iexit 10 AOKXC MemJKOP . 2048 crit_e 1.d-4 $END $TDDFT isoc 2 nfiles 2 ifgs 1 imatsoc 1 0 0 0 2 1 1 $END }}} = Output = * ** List of SOC-SI results *** Totol No. of States: 41 . No. ExEnergies f Dominant Excitations Esf dE Eex(eV) (cm^-1) . 1 -0.0066 eV 0.0000 99.8% Spin: |Gs,1> 0-th A 0.0000 -0.0066 0.0000 0.00 2 2.5694 eV 0.0000 44.1% Spin: |S+,2> 1-th A 2.6425 -0.0731 2.5760 20776.65 3 2.5727 eV 0.0000 32.8% Spin: |S+,3> 1-th A 2.6425 -0.0698 2.5793 20803.69 4 2.5908 eV 0.0000 31.8% Spin: |S+,1> 1-th A 2.6425 -0.0517 2.5974 20949.77 5 2.7010 eV 0.0000 31.1% Spin: |So,1> 1-th A 2.9592 -0.2583 2.7076 21837.87 6 2.8740 eV 0.0000 19.9% Spin: |S+,1> 2-th A 2.9081 -0.0340 2.8806 23233.61 7 2.8794 eV 0.0000 27.0% Spin: |S+,2> 2-th A 2.9081 -0.0287 2.8859 23276.69 8 2.9589 eV 0.0000 22.8% Spin: |S+,1> 3-th A 2.9849 -0.0261 2.9655 23917.99 9 3.0395 eV 0.0000 26.0% Spin: |S+,2> 2-th A 2.9081 0.1314 3.0461 24568.13 . 10 3.0631 eV 0.0000 38.7% Spin: |S+,2> 3-th A 2.9849 0.0782 3.0697 24758.84 11 3.0881 eV 0.0000 52.9% Spin: |So,1> 2-th A 3.0330 0.0551 3.0947 24960.28 12 3.1239 eV 0.0000 30.7% Spin: |So,1> 1-th A 2.9592 0.1647 3.1305 25249.42 13 3.1328 eV 0.0000 21.9% Spin: |S+,2> 5-th A 3.1710 -0.0382 3.1394 25320.98 14 3.1334 eV 0.0000 20.5% Spin: |S+,3> 4-th A 3.1640 -0.0305 3.1400 25325.94 15 3.1455 eV 0.0000 33.3% Spin: |S+,2> 4-th A 3.1640 -0.0185 3.1521 25423.24 16 3.1489 eV 0.0000 24.5% Spin: |S+,2> 5-th A 3.1710 -0.0221 3.1555 25450.64 17 3.1546 eV 0.0000 17.0% Spin: |S+,3> 4-th A 3.1640 -0.0094 3.1612 25496.52 18 3.1580 eV 0.0000 34.2% Spin: |S+,3> 5-th A 3.1710 -0.0130 3.1646 25524.02 19 3.1866 eV 0.0000 17.4% Spin: |S+,2> 7-th A 3.2865 -0.1000 3.1932 25754.60 20 3.2140 eV 0.0000 28.2% Spin: |S+,3> 6-th A 3.2065 0.0074 3.2206 25975.68 21 3.2174 eV 0.0000 48.4% Spin: |S+,2> 6-th A 3.2065 0.0109 3.2240 26003.33 22 3.2435 eV 0.0000 38.0% Spin: |So,1> 3-th A 3.2231 0.0204 3.2501 26213.63 23 3.2627 eV 0.0000 20.7% Spin: |S+,3> 6-th A 3.2065 0.0562 3.2693 26368.83 24 3.2725 eV 0.0000 30.0% Spin: |S+,2> 7-th A 3.2865 -0.0140 3.2791 26447.54 25 3.3035 eV 0.0000 45.4% Spin: |So,1> 3-th A 3.2231 0.0804 3.3101 26697.85 26 3.3651 eV 0.0000 23.9% Spin: |So,1> 4-th A 3.5132 -0.1481 3.3717 27194.63 27 3.3945 eV 0.0000 31.5% Spin: |S+,1> 8-th A 3.4260 -0.0315 3.4011 27431.99 28 3.4070 eV 0.0000 31.1% Spin: |S+,1> 9-th A 3.4454 -0.0384 3.4136 27532.74 29 3.4308 eV 0.0000 31.7% Spin: |S+,3> 8-th A 3.4260 0.0047 3.4374 27724.20 30 3.4465 eV 0.0000 19.7% Spin: |S+,2> 8-th A 3.4260 0.0204 3.4531 27850.76 31 3.4518 eV 0.0000 55.5% Spin: |S+,2> 8-th A 3.4260 0.0257 3.4583 27893.46 32 3.4658 eV 0.0000 43.7% Spin: |S+,2> 9-th A 3.4454 0.0204 3.4724 28006.99 33 3.4764 eV 0.0000 24.6% Spin: |S+,1> 10-th A 3.4870 -0.0106 3.4830 28092.46 34 3.5252 eV 0.0000 68.4% Spin: |S+,2> 10-th A 3.4870 0.0382 3.5318 28485.50 35 3.6092 eV 0.0000 49.3% Spin: |So,1> 4-th A 3.5132 0.0960 3.6158 29163.42 36 3.6402 eV 0.0000 60.5% Spin: |So,1> 6-th A 3.5920 0.0482 3.6468 29413.12 37 3.6508 eV 0.0000 48.8% Spin: |So,1> 5-th A 3.5648 0.0859 3.6574 29498.52 38 3.6609 eV 0.0000 47.4% Spin: |So,1> 7-th A 3.6206 0.0403 3.6675 29580.42 39 3.6684 eV 0.0000 43.5% Spin: |So,1> 8-th A 3.6288 0.0396 3.6750 29640.60 40 3.7293 eV 0.0000 83.7% Spin: |So,1> 9-th A 3.6898 0.0395 3.7359 30131.95 41 3.7898 eV 0.0000 90.1% Spin: |So,1> 10-th A 3.7487 0.0411 3.7964 30620.26 Print selected matrix elements of [Hsoc] < 0 0 0 |Hso| 2 1 1 > mi/mj ReHso(au) cm^-1 ImHso(au) cm^-1 . 1 1 0.0003219734 70.6650036601 0.0009582030 210.3012602778 1 2 0.0000000000 0.0000000000 -0.0006544171 -143.6279497862 1 3 0.0003219734 70.6650036601 -0.0009582030 -210.3012602778 [tddft_soc_final] |
== Stability analysis == === isab === === isave === == memory control == === memjkop === == Others == === isgn === === ivo === |
tddft: time-dependent density functional theory
Contents
Time dependent DFT/HF calculation. Support Full TDDFT, TDA and RPA.
Quick guides
The following examples give the minimal inputs for starting TD-DFT calculations.
1. Closed-shell Systems : R-TD-DFT
2. Open-shell Systems : U-TD-DFT and spin-adapted TD-DFT for spin-conserving excitations
3. Open-shell Systems : Spin-flip TD-DFT for spin-flip excitations
General keywords
imethod
isf
itda
idrpa
ispa
ialda
thrdab
itest
icorrect
itrans
iro
icv
ioo
iksf
iact
elw
eup
idiag
ndiag
aokxc
Convergence threshold
crit_e
crit_vec
States specification
iext
next
Save eigenvectors
istore
Integer: specify the file no. to store TDDFT information
lefteig
By default, in TD-DFT the left eigenvector X-Y is also stored.
output eigenvector control
nprt
cthrd
TD-DFT/SOC and Property evaluation
nfiles
No. of TD-DFT calculations to be loaded.
isoc
=1, Only work for closed-shell case (NOT recommended!)
=2, General SOC state interaction
=3, just print SOC matrix elements between two spin-free states (without diagonalization Hsoc).
ifgs
=0, default for not including ground state (GS) in SOC treatment; =1, include GS.
imatsoc
Define SOC matrices need to be calculated. Input format looks like
... #SCF calculation for the ground state S0. It is a singlet. $scf spin 0 ... $end #First TDDFT, singlets S0-S9. $tddft imethod 1 isf 0 iext 10 .... $end #Second TDDFT, triplet T1-T10 $tddft imethod 1 isf 1 iext 10 $end $tddft .... imatsoc 7 0 0 0 2 1 1 0 0 0 2 1 2 1 1 1 2 1 1 1 1 1 2 1 2 1 1 2 2 1 1 1 1 2 2 1 2 2 1 1 2 1 1 2 1 1 2 1 2 $end
In this input, 7 means seven of SOC matrices will be calculate (If the number <0, then ALL possible HSOC mat will be printed !). Here, it is very tricky to specify states:
- The string "0 0 0" always treat as the ground state.
For other states, three numbers "n m n" represent "ith-tddft", "symmetry" and "ithstate" respectively. Therefore, the first matrix element "0 0 0 2 1 1" means SOC matrix of <S0|HSOC|T1>. The third matrix element "1 1 1 2 1 1" means SOC matrix <S1|HSOC|T1>. Here, the first "1" in bra state "1 1 1" means the state from first TDDFT calculation. The second and third "1" in the bra state "1 1 1" means this state has spatial symmetry "1" and is the first excited state.
imatrsf
Transition dipole between Spin-free states. The input is similar to imatsoc (but currently selected printing is not implemented). Simply use -1 to print all of them.
imatrso
Define transition dipole moment need to be printed between two SOC-included states. Input format looks like(notice we omit other input in TDDFT module)
$TDDFT ... imatrso 5 1 1 1 2 1 3 1 4 1 5 ... $END
Then, "imatrso" is specified to define transition dipole moments need to be printed. The number "5" require transition dipoles between 5-pairs of states to be print. The following 5 lines define which pairs will be printed. Here, we require transition dipoles between the first state and five states are printed.
idiag
By default, idiag=0 uses full diagonalization (preferred for small model space).
If idiag=1, then TD-DFT/SOC can use Davidson's algorithm also, along with a specification for the no. of states by iexit.
iact
=1, allows to use active space specification for the projected active-orbital SOC Hamiltonian (P*HSOC*P), eup can be specified in (eV) to give a cut off to define active physically interested excited states.
Stability analysis
isab
isave
memory control
memjkop
Others
isgn