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GIF89ah1w !ÿ NETSCAPE2.0 !þ4Created by Wolfram Mathematica 9.0 : www.wolfram.com !ù , h1$$$%%%&&&'''((()))***+++,,,---...///000111222333444555666777888999:::;;;<<<:>>;@@:??===>>>???@@@Tr _f ,Y';x#5l 1b>BBAAABBBCCCDDDBGGEEEFFFGGGHHHFLLIIIJJJKKKLLLMMMNNNOOOPPPJPPKQQNTTOUUQQQRRRSSSTTTUUUVVVWWWXXXRXXSZZW^^U[[YYYZZZ[[[\\\]]]^^^___```Y``[bb_gg]ddaaabbbcccdddeeefffggghhhahhckkgooiiijjjkkklllmmmnnnooopppjrrnvvluunwwqqqrrrssstttuuuvvvwwwxxxr{{u~~yyyzzz{{{|||}}}~~~±-+%#Ó53î<:ÿUR¨ýÿ'þÿ,õý&ÿÿ6çõ#ÑàÜã<0I8T«=[¹5P¢BcÊGkÙNtëS|úNuë<Zµz~{ |
= First-order nonadiabatic couplings = The calculations of first-order nonadiabatic couplings between ground and excited-states ('''<0|Dx|Sn>'''), and those between the excited-states ('''<Sm|Dx|Sn>''' or '''<Tm|Dx|Tn>''') at the TD-DFT/TDA level can be achieved by generalizing the standard linear and quadratic response theories, for details, see |
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x\ÿdÿmÿiþx§ÿ | ''Zhendong Li and Wenjian Liu, "First-order nonadiabatic coupling matrix elements between excited states: A Lagrangian formulation at the CIS, RPA, TD-HF, and TD-DFT levels", J. Chem. Phys. 141, 014110 (2014). '' |
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For convenience, however, in the input they are both specified by the '''QUAD''' keyword with '''single''' and '''double''', respectively. Either analytic derivative or finite difference approach can be used. The latter is only allowed for C(1) symmetry, and for molecules without orbital degeneracy! |
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¢¢§§¦¦¤¤ªª ¡¡¡¤¤¤¦¦¦¨¨¨¢¯¯ªªª©©©«««°°°¦³³§´´ª··®»»³³³···²¿¿»»»¾¾¾¶ÄÄÀÎμË˹ÇÇÌÿÄÄÄÊÊÊÎÎÎÂÐÐÃÒÒÇÖÖÅÔÔÉØØËÚÚÐßßÎÞÞÍÛÛÕØØÓââ×ççÕååÛëëÞïïÝììÙèèàññäôôìøøõüüÿÿÿýÿÿûþþó÷÷ãîîµôz þ í H° Á*\Ȱ¡Ã#JH±¢Å3jÜȱ£Ç C I²¤É(Sª\ɲ¥Ë0cÊI³¦Í8sêÜɳ§Ï@ |
== Analytic derivative approach == |
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J´¨Ñ£H*]Ê´©Ó§P£JJµªÕ«X³jÝʵ«×¯`à K¶¬Ù³hÓª]˶۷pãÊK·®Ý»xóêÝË·¯ß¿ |
== Finite difference approach == {{{ $COMPASS Title nh3 Basis sto-3g Geometry C 0.00000000 -1.20809142 -1.14173975 C 0.00000000 -1.20797607 0.25342015 C 0.00000000 0.00000000 0.95085852 C -0.00000000 1.20797607 0.25342015 C -0.00000000 1.20809142 -1.14173975 C 0.00000000 0.00000000 -1.83922155 H 0.00000000 -2.16045397 -1.69142002 H 0.00000000 -2.16044427 0.80300713 H -0.00000000 2.16044427 0.80300713 H -0.00000000 2.16045397 -1.69142002 H 0.00000000 0.00000000 -2.93882555 F 0.00000000 0.00000000 2.30085848 End geometry skeleton group c(1) nosym $END |
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$xuanyuan direct schwarz $end |
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QRÑÂÛÃv鮩 | $scf RHF charge 0 spin 1 THRESHCONV 1.d-10 1.d-8 OPTSCR 1 iaufbau 0 $end |
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ÍÜP/4R ã¹ ³ Î-¥Ã§.Q@M]д»®º-®°[·Ò³ p;aNÑÈwÈg&*í¨ Lî±F ÿQäVÁY^ciP8I`.<[ؽÕ`ËËÄMB¤-S T gÓÒd2Ý9?µ 7¦ã*þiæ&>ðÄð!~ª¹ À 1p´mLÇxâjbfG%¨.ðË6 ùt Õ@HÉ®I ·Ê£b+1 L,è v0 ð èêT±; Ä@ÓÆÐ0q á14s$D¤.n<.3&qP¬&«+næP)O¿| ÊÀó Ô òW ¯@Ç AÉu7¯WbTòå HçÛ$w ë)¡{Û°í°p ºÇ{óÀTgÉq|?U@æj©Pg÷~NZ©0Ë 0ñ&EÊ ô0èðÙ Òpê à³ÌÅþÜZ;^õU0 #V,Î[ð"É/1· =:Z°¹ïB éÆzÊ ¸Ö kÑ àüAÙ%!;.®úNäoD#òª Ñâ{ |
$tddft imethod 1 isf 0 iexit 2 itda 1 idiag 1 istore 1 crit_e 1.d-10 crit_vec 1.d-8 lefteig AOKXC DirectGrid $end |
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DPáBu|¥,]¾p -ZÔ`$M¦Y=~RäÈhtIu ÔÈZ.ü(òäÌF6H-¹u,ÕE^ ñÖk¯JÅé¢ÂèÔv¨ULZ1ª YôÒUìX² Ô(cëØJ4ÙóãÉ8e/6ÀÙ B ZîyF«]Â"¨Ôo·ö´©Axä _,eYóf ´þñ¥Í=DF¨¸Z3¡l94Ð@ Ü(Zº$hñ¤Í.¡¦_ÏÄIlºÇ´@Å!øû" I?N8BwJJµa(µ]¦ncÌ7ãm Ð CðR (j¯\G¿k9tèÖÅy¢.´?D¬ÜÊ8æj³Í6ÔB|êB±o^Ù£ èM'üÒ"½Ü@3¦!´´º´§bÂyG wÂ!¦"~±G\¨ S¹Å_´¨»¹¨+b0+Ã]îh# üpJ ÜD K©á-ë®óÍÀ Ô Æ|ìqgz2N9aTþoÅÑVâj TÀàôf{BÂ(x±Ë"ºH R£cI¥¡Y¤ÑÆ t²É©2ç$µÔÍ KJ2@¥ "h Öf5 ôÖk/ÏÁzL/µ;â ³ ñ¾ìE5è¡YÙ&\â¸åM¥¶Z» @» £(°!¸`§ù¼ÙµGTøéÂ"X¬a'1¿DËH Tde@/µ¶_· Ú좼ÎêgîK°¯Ôò:2%eÂ1ç9 H Ù)¾è¢÷ê_Oö(¯p1)Êð q4 ¶ÙÒKâ4ráÆwÜþù-¤ºx¦æ&£pE¹i§Ä¢ |èÉH«A¯vÞ¦ yfæì°!º(§Jù5ûé Ýív&) û ATZ4ÐS{ÚÑfc%ø8¨yÆð¸wZè i/Ùa|Ä o# dsáte* µ¬D¢RërÙM®' j51'tÚ!;AÃnm$ê`,yÆ©äìÂàh¢¶ë=ûRÏL^®N°dqêÁÇ iíKÐ3@ ªHã _{°¢X \ÚÍS{ÿKM dtå ¹ÈÆ:þÇ ^ èË Ú°kìâ1v¡AJ±Pܦo* ÆÿD¤LH!¹¡Xbd áPƤ pÕ \hÃ-RÔ ZJ ¢|A #D"Ò0£äåb,,¨B&Q bXbN7ip°.i¡N Uj WÜZ \Õ %¦øhÇ45Ø¡¥2Âj ê´îÍHÃXÒ W(F 4Xc"TYLcfæFYb@- qi-xh|!í¤ 8ÄPö (ÒÒA H i âÉËÛìa /uáÍØEýB¢D ÂwBÉNþ9LåPF |
$resp iprt 1 QUAD FNAC single states 1 1 1 2 double pairs 1 1 1 1 1 1 2 norder 1 method 2 nfiles 1 FDIF step 0.001 ignore 1 noresp $end }}} To use finite-difference, a script '''fdiff.py''' should be used as |
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Á 1 í¡¾ü>xéKC@A×TN l.5Q@"ÄiRPD7Õ¹N èå8ɹEâédg>õùbâ¦"@YBÔÓ@'>ö¹PÚEýT@áÏB Ô¢H"ÚPv´( }(<'*P{R¡ÈÇ=ºR¤i<Pòm´¥7Å©BB*RúR¥9jPí!~ø3(:|Y¡65§; §!jD8Õª-%*D zTB\Õ« }¨ ñAB]ýjZ÷z<t¬ZÕ:W}5p]õºþN|¼µ¬eÝk`± b D^»ØD¬,c%Äàp 6";YÎjÅìf;;Ú¸À´ýÃeñÒ¶n=íXSëZÚ6í³8meaÓÚöZø8mjïzWß×Z±Mí a\æ ¸%ìr;]RÖ ¼¥nvµ»]îv×»ßoxÅ;^ò×¼çEozÕ»^ö¶×½ï o|å;_úÖ×¾÷Åo~õ»_þö׿ÿp<`ØÀFp¼`7ØÁp%<a WØÂÆp5¼awØÃqE<bØÄ'FqU¼b·ØÅ/qe<c%רÆ7Æqu¼c ÷ØÇ?r <d"ÙÈGFr¼d&û7 !ù , h1$$$%%%&&&'''((()))***+++,,,---...///000111222333444555666777888999:::;;;<<<:>>;??===>>>???@@@Sr ^e +W';x#4j 0a>CCAAABBBCCCDDDBGGEEEFFFGGGHHHIIIJJJKKKLLLJOOMMMNNNOOOPPPGLLNSSNTTQQQRRRSSSTTTUUUVVVWWWXXXQXXSZZW^^U\\YYYZZZ[[[\\\]]]^^^___```Y``[bb^eeaaabbbcccdddeeefffggghhhahhcjjgooelliiijjjkkklllmmmnnnooopppkssnwwluupyyqqqrrrssstttuuuvvvwwwxxxr{{vyyyzzz{{{|||}}}~~~±-+%#à96þTRýÿ'þÿ,õý%ÿÿ6ç÷#ÓãÀÉ,0H8T«=[¹5P¢BcÉGj×MtêT~üRzõNtë<Yµz}}^ÿZ þgÿlþy¨ÿ |
{{{ ./fbdiff.py run.sh input.inp > log }}} After the calculation is done, an output file '''input.out''' will present in the current directory. The '''log''' file saves the information during the calculations. |
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