FUNCTION GROUND(RHH,RLIHA,RLIHB) CCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCC C C THIS ROUTINE COMPUTES THE POTENTIAL ENERGY VALUES C OF THE GROUND ELECTRONIC STATE OF THE LIH2+ SYSTEM C AS EXPLAINED IN DETAIL IN C C R. MARTINAZZO, G.F. TANTARDINI, E. BODO, F.A. GIANTURCO C J. CHEM. PHYS. 119 (2003) 11241 C C ON INPUT C RHH, RLIHA, RLIHB ARE THE H-H AND LI-H INTERNUCLEAR DISTANCES C IN ATOMIC UNITS C ON OUTPUT C GROUND IS THE TOTAL ENERGY (IN ATOMIC UNITS) REFERRED TO THE C THREE-BODY BREAK-UP ASYMPTOTE C C CALL IT AFTER AN INITIALIZATION CALL TO GROUND_I C USE YOUR OWN 2-BODY POTENTIAL, IF DESIRED, BY CHANGING C H2_KW AND XLIH_FCI FUNCTIONS C C LIST OF SUBROUTINES AND FUNCTIONS: C C SUBROUTINE GROUND_I INIZIALIZATION C FUNCTION V3BODY 3-BODY POTENTIAL C FUNCTION H2_KW H2 GROUND-STATE POTENTIAL C FUNCTION XLIH_FCI LIH+ GROUND-STATE POTENTIAL C FUNCTION H2QUAD HH QUADRUPOLE C FUNCTION H2POL HH SPHERICAL, '3-BODY' POLARIZABILITY C FUNCTION H2POL2 HH ANYSOTROPIC POLARIZABILITY C CCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCC IMPLICIT NONE DOUBLE PRECISION RHH,RLIHA,RLIHB DOUBLE PRECISION POT,V3BODY,H2_KW,XLIH_FCI DOUBLE PRECISION GROUND POT=V3BODY(RHH,RLIHA,RLIHB) POT=POT+H2_KW(RHH)+XLIH_FCI(RLIHA)+XLIH_FCI(RLIHB) GROUND=POT END SUBROUTINE GROUND_I INTEGER MMAX,MLONG,MA PARAMETER (MMAX=10,MLONG=1,MA=143) INTEGER NDIM,NEXP1,NEXP2,NEXP3 COMMON/DIM/ NDIM(MMAX) COMMON/EXP1/ NEXP1(MA-2-MLONG) COMMON/EXP2/ NEXP2(MA-2-MLONG) COMMON/EXP3/ NEXP3(MA-2-MLONG) INTEGER MAL,I,J,K,M,JJ,KK,IM NDIM(1)=0 JJ=0 DO M=2,MMAX KK=0 DO I=0,M DO J=0,M C DO K=0,M C MODIFICATIONS FOR AB2 SYSTEMS ----> K.LE.J C FOR A3 SYSTEMS ----> K.LE.J.AND.I.LE.J DO K=0,J IM=I+J+K IF(IM.EQ.M)THEN IF(I.NE.M.AND.J.NE.M.AND.K.NE.M)THEN JJ=JJ+1 KK=KK+1 NDIM(M)=KK NEXP1(JJ)=I NEXP2(JJ)=J NEXP3(JJ)=K ENDIF ENDIF ENDDO ENDDO ENDDO WRITE(*,*)'ORDER...',M WRITE(*,*)'NUMBER OF TERMS...',NDIM(M) WRITE(*,*)'EXPONENTS..' DO KK=1,NDIM(M) WRITE(*,*) NEXP1(JJ-NDIM(M)+KK), & NEXP2(JJ-NDIM(M)+KK), & NEXP3(JJ-NDIM(M)+KK) ENDDO ENDDO RETURN END FUNCTION V3BODY(R1,R2,R3) IMPLICIT NONE DOUBLE PRECISION R1,R2,R3,V3BODY INTEGER MMAX,MLONG,MA,NSW PARAMETER (MMAX=10,MLONG=1,MA=143,NSW=2) INTEGER NDIM,NEXP1,NEXP2,NEXP3 COMMON/DIM/ NDIM(MMAX) COMMON/EXP1/ NEXP1(MA-2-MLONG) COMMON/EXP2/ NEXP2(MA-2-MLONG) COMMON/EXP3/ NEXP3(MA-2-MLONG) DOUBLE PRECISION A(MA) DATA A/ 59.9041369487, & -4.4190710855, & -1793.3690652080, & -92.7339536285, & 231.0047518887, & 23.6312294844, & 42386.6962109884, & 20887.4910336156, & -101.8488429800, & -4783.2820589398, & 5601.4299484618, & 647.9336802252, & -2188.0964589478, & -333391.4339867483, & -50650.0836783211, & -216249.6666120038, & -10968.2992516742, & 14746.3468957760, & 64623.8750484771, & -6585.4074148974, & -121946.1513253672, & 2470.5168826501, & 39388.8512400949, & 674663.0178284654, & -623209.8463494780, & -625800.6376789842, & 5061315.2544497522, & -499972.9861830364, & 738165.5689500275, & -3062084.0673502581, & -890975.0918916499, & 37100.2541750794, & 481176.7795094966, & 68335.2125605610, & 860916.1659883368, & -182446.6634467566, & -313469.8588537204, & 16296025.2245538831, & 24283257.8151341975, & 2226423.3841185221, & -55670137.2963673249, & -41861251.3156600073, & 12522078.8982328828, & -10780744.6234461721, & 19920454.5483050309, & 3725852.5719358511, & -888096.4455630139, & 5805044.5654820763, & -1174676.0747827506, & -152672.8060593364, & -3582082.6546327011, & 252873.3936963925, & -3291637.8143871599, & 1409200.5075722407, & 1356914.6186123572, & -79156096.6236694306, & -134289948.7898918688, & -144168137.8314403296, & 18010795.4982191287, & 184494908.8457103074, & 201704765.4667312205, & -99315107.5417414308, & 64030848.3463394046, & 62186512.0140229985, & -69323914.7188201100, & -18225109.7742339559, & 8767846.0950237475, & -71368402.0258482397, & 20651551.6130857319, & 1535688.4530311411, & 12342388.8021743763, & 5825471.3843415780, & -3734791.5687767509, & 10453889.2599439640, & -704923.1248095465, & 7092463.0621291548, & -5229921.5270726196, & -3297509.8045103801, & 170414954.6685615480, & 442318060.4571669102, & 338310296.6504344344, & -106295716.0848532170, & -243177154.1358072460, & -272160559.5405060053, & -560001873.6517249346, & 345105141.7074456215, & -179453069.6148003042, & -205181566.6644286513, & 178625484.6556275785, & 80765193.6117105931, & -34816331.7087118998, & -22162585.9540813640, & 117201851.0785028338, & -94646151.0332854241, & -10872024.4385482874, & 134794077.4815447628, & -23336856.3831176758, & 15174814.7355045378, & -78927252.4897296727, & -12871086.9000668079, & 4843936.1891660253, & -11668605.0056117158, & 426732.0261371761, & -8474699.3137837537, & 9738486.1953393687, & 4215023.2278999090, & 83709195.3309966177, & -81955642.6349996924, & -509178802.8625016212, & -253164045.3674562573, & 145445180.5049311221, & -261403144.5543840528, & -214500767.8142659366, & 597722827.9000399113, & -439796210.5928990245, & 195491463.8727613091, & 412858125.1965236664, & 989693212.4453485012, & 179744133.8334875405, & -158573195.2249470055, & 47721187.7360739559, & -309115588.9086966515, & -865951061.6187733412, & 103449948.7291473746, & 25790340.4448547661, & 33253194.3017021790, & 415688777.1302601099, & 169521356.8767541051, & -23916729.3615326211, & -214129802.4606905282, & -89171572.5754874349, & -11048394.8646354862, & 122655134.3360205442, & 37156079.7304429114, & 1487230.4260974966, & -1885306.1160342137, & -502645.5527109082, & 5039172.7627611337, & -7203742.8395571373, & -2200156.4276824687, & 1.0277126653, & 1.4179477712, & 2.5479621480/ DOUBLE PRECISION BETA1,BETA2,BETA3 DOUBLE PRECISION RO1,RO2,RO3 DOUBLE PRECISION RHO1,RHO2,RHO3,RHO_0,RHOU DOUBLE PRECISION YMOD,DYDA DOUBLE PRECISION RSCAT,COSANG DOUBLE PRECISION FACTOR,DENOM,VLONG,V3B DOUBLE PRECISION Q,DELALP_0,ALP_2,P2 DOUBLE PRECISION H2POL,H2POL2,H2QUAD INTEGER MAL,I,J,K,M,JJ,KK,IM,N1,N2,N3 C MAL=MA-3 C AB2 SYSTEM MAL=MA-2-MLONG BETA1=A(MAL+1) C AB2 SYSTEM BETA2=A(MAL+2) BETA3=A(MAL+2) C LONG-RANGE PARAMETERS RHO_0=ABS(A(MA-MLONG+1)) RO1=R1 RO2=R2 RO3=R3 RHO1=RO1*DEXP(-BETA1*RO1) RHO2=RO2*DEXP(-BETA2*RO2) RHO3=RO3*DEXP(-BETA3*RO3) YMOD=0.0D0 JJ=0 DO M=2,MMAX DO KK=1,NDIM(M) JJ=JJ+1 N1=NEXP1(JJ) N2=NEXP2(JJ) N3=NEXP3(JJ) IF(N2.EQ.N3)THEN DYDA=RHO1**N1*RHO2**N2*RHO3**N3 ELSE DYDA=RHO1**N1* & (RHO2**N2*RHO3**N3+ & RHO2**N3*RHO3**N2) ENDIF YMOD=YMOD+A(JJ)*DYDA ENDDO ENDDO C ----------------------------------------------------------- C LONG-RANGE TERM EVALUATION C C LONG-RANGE CONTRIBUTIONS FOR ARRANGEMENT 1, HH--LI C RSCAT IS THE SCATTERING COORDINATE IN THIS C ARRANGEMENT AND COSANG IS THE COSINE OF C THE JACOBI ANGLE C C LI C /| C / | C R2 / | R3 C / | C / THETA C H------H C R1 RSCAT=DSQRT(0.50D0*R2**2+0.50D0*R3**2+ & -0.25D0*R1**2) COSANG=(R2**2-R3**2)/R1/RSCAT/2.0D0 C COMPUTE SWITCHING FUNCTION IF(RSCAT.LT.RHO_0)THEN FACTOR=0.0D0 DENOM=1.0D0 VLONG=0.0D0 V3B=YMOD ELSE RHOU=RHO_0/RSCAT DENOM=1.0D0/(1.0D0-(RHOU)**NSW) FACTOR=EXP(1.0D0)*EXP(-DENOM) C C COMPUTE HH QUADRUPOLE AND POLARIZABILITY FOR R=RHH C Q IS THE QZZ COMPONENT OF THE QUADRUPOLE TENSOR C C ALP_0=1/3 *(ALPHA_XX+ALPHA_YY+ALPHA_ZZ) C AND C POL2=(ALP_ZZ-ALPHA_0) C C POL = ALP_0-2.0*ALPHA_H C C P_0(X)=1, P_2(X)=1/2*(3*X**2-1) C Q=H2QUAD(R1) DELALP_0=H2POL(R1) ALP_2= H2POL2(R1) P2=0.5*(3*COSANG**2-1.0) VLONG= Q*P2/RSCAT**3 + & -DELALP_0/2.0D0/RSCAT**4 + & -ALP_2*P2/2.0D0/RSCAT**4 V3B=YMOD*(1.0D0-FACTOR) + VLONG*FACTOR ENDIF C C END OF TOTAL LONG-RANGE POTENTIAL EVALUATION C -------------------------------------------------------------- V3BODY=V3B RETURN END FUNCTION H2QUAD(R) IMPLICIT DOUBLE PRECISION(A-H,O-Z) DOUBLE PRECISION H2QUAD C C HYDROGEN QUADRUPOLE (A.U.) C AS A FUNCTION OF THE INTERNUCLEAR C DISTANCE (A.U.) C STANDARD DEVIATION: 0.000325557608 C PARAMETER(NA= 4) DIMENSION A(NA),FACT(2) DATA A / & -0.0126271402, & +0.341987071, & -0.0249680149, & +0.000251740527/ DATA BETA/ 0.0673276303/ DATA FACT/ 1.3899166, 3.30599025/ DESP=DEXP(-BETA*R) RHO=R*DESP DUXPO=DEXP(FACT(1)*(R-FACT(2))) FACTOR=1.0D0/(1.0D0+DUXPO) YMOD=0.0D0 DO M=1,NA YMOD=YMOD+A(M)*RHO**M ENDDO H2QUAD=YMOD*FACTOR RETURN END FUNCTION H2POL(R) IMPLICIT DOUBLE PRECISION(A-H,O-Z) DOUBLE PRECISION H2POL C C FULLCI H(Liu-augaug) C HYDROGEN 3-BODY C SPHERICAL POLARIZABILITY (A.U.) C DALPHA_0=ALPHA_0-2*ALPHA_H C AS A FUNCTION OF INTERNUCLEAR C DISTANCE (A.U.) C STANDARD DEVIATION = 0.00741821229 C PARAMETER(NA= 4) DIMENSION A(NA),FACT(2) DATA A / & +0.0682048466, & +1.69575813, & -0.0379060701, & +0.0149673329/ DATA BETA/ 0.0567659808/ DATA FACT/ 1.55657199, 3.19559801/ DESP=DEXP(-BETA*R) RHO=R*DESP DESP1=DEXP(- 0.0724081327*R) DUXPO=DEXP(FACT(1)*(R-FACT(2))) FACTOR=1.0D0/(1.0D0+DUXPO) YMOD=0.0D0 DO M=1,NA YMOD=YMOD+A(M)*RHO**M ENDDO YMOD=YMOD+ -7.4989518*DESP1 H2POL=YMOD*FACTOR RETURN END FUNCTION H2POL2(R) IMPLICIT DOUBLE PRECISION(A-H,O-Z) DOUBLE PRECISION H2POL2 C C FULLCI H(Liu-augaug) C HYDROGEN ANISOTROPIC C POLARIZABILITY (A.U.) C ALPHA_2=ALPHA_ZZ-ALPHA_0 C AS A FUNCTION OF INTERNUCLEAR C DISTANCE (A.U.) C C STANDARD DEVIATION= 0.00863041785 C PARAMETER(NA= 5) DIMENSION A(NA),FACT(2) DATA A / & 0.0266251827, & 0.139081715, & 0.324064812, & -0.0511107403, & 0.00279102422/ DATA BETA/ -0.0729582362/ DATA FACT/ 1.59140975, 3.1416315/ DESP=DEXP(-BETA*R) RHO=R*DESP DUXPO=DEXP(FACT(1)*(R-FACT(2))) FACTOR=1.0D0/(1.0D0+DUXPO) YMOD=0.0D0 DO M=1,NA YMOD=YMOD+A(M)*RHO**M ENDDO H2POL2=YMOD*FACTOR RETURN END C C ---- 2-BODY POTENTIALS FOLLOW ------- C FUNCTION H2_KW(R) C C FITTING OF THE KOLOS & WOLNIEWIC C PEC FOR THE H2 MOLECULE C FINAL STANDARD DEVIATION: 3.27320215E-05 A.U. C (i.e. 7.2 CM-1) C IMPLICIT DOUBLE PRECISION(A-H,O-Z) PARAMETER(NA= 8) DIMENSION A(NA),FACT(2) DATA A / & -0.142978719, & -17.4496708, & 215.8658, & -1763.38375, & 9338.55361, & -30639.411, & 56147.2305, & -43929.2685/ DATA BETA/ 1.19999843/ DESP=DEXP(-BETA*R) RHO=R*DESP FACTOR=1.0D0 YMOD=0.0D0 DO M=1,NA YMOD=YMOD+A(M)*RHO**M ENDDO DESP1=DEXP(- 1.2*R)/R YMOD=YMOD+ 0.637669117*DESP1 H2_KW=YMOD*FACTOR RETURN END FUNCTION XLiH_FCI(R) C C Fitting of the LiH+ FullCI curve C with the Li(Y)+H(Liu-augaug) C basis-set. All values are in a.u.. C C STANDARD DEVIATION = 3.17247272E-05 C (i.e. 6.96 cm^-1). C IMPLICIT DOUBLE PRECISION(A-H,O-Z) PARAMETER(NA= 6) DIMENSION A(NA),FACT(2) DATA A / & -0.436998324, & -10.9156475, & 55.0379023, & -437.23156, & 1443.14556, & -2340.82341/ DATA BETA/ 1.00000006/ DATA FACT/ 5.85874466, 1./ DESP=DEXP(-BETA*R) RHO=R*DESP FACTOR=1.0D0 factor1=0.0d0 rhou= 5.85874466/R if(rhou.lt.1.0d0)then factor1=dexp(-1.0d0/(1.0d0-rhou** 2)) factor1=factor1*dexp(1.0d0) endif YMOD=0.0D0 DO M=1,NA YMOD=YMOD+A(M)*RHO**M ENDDO DESP1=DEXP(- 1.*R)/R YMOD=YMOD+ 16.1279348*DESP1 VLONG=- 4.5/2.0D0/R**4 YMOD=YMOD*(1.0d0-FACTOR1)+FACTOR1*VLONG XLIH_FCI=YMOD*FACTOR RETURN END