! file: label.dat ! label.dat is an input to SHELL ! When SHELL is run, the following combinations of ! model-space and interaction can be specified. A new combination ! of names will be given the default code x for the model space and ! y for the interaction. ! ! IMPORTANT: If you change one or more of the two-body ! matrix elements in a *.INT file be sure to ! delete *.opn file and rerun shell so that a new *.opn ! file will be made ! !(1) Model space (*.SP file) name (single-particle state file name) !(2) Interaction (*.INT file) name ! In some cases the interaction may consist of several pieces ! which are read into MATRIX separately. In this case this ! interaction name is the code word which tells SHELL ! which *.INT files to include.) !(3) Model space code used for the output files ! (The labels "p" and "n" should be reserved for charge-dependent ! interations names) !(4) Interaction code used for the output files !(5) References and information ! ! Reference list for model spaces (* is reserved) ! (3) (1) (3) (1) (3) (1) (3) (1) ! a p,ppn h ho,f5p o v jj56pn,jj67pn,PBPOP ! b sd,sdpn,sdw i gl,jj45 p * w pb206 ! c zbm,zbmpn,zbme j slg q jj55pn x * ! d psd,psdpn k sns r jj45pn y ! e f7,f7pn l sdpf,sdpfpn s z ! f fp,fppn m n82 t SPSDPF ! g d3f7,d3f7pn n * u i13 ! list of available model-space and interaction combinations ! ---------------------------------------------- !(1) (2) (3) (4) (5) ! ---------------------------------------------- ! P Model Space ! 1p1/2,1p3/2 orbits p ckpot a a ! (8-16)POT S. Cohen and D. Kurath, p cki a b ! (6-16)TBME Nucl. Phys. A73, 1 (1965) and p ckii a c ! (8-16)TBME Nucl. Phys. A101, 1 (1967) p pmom a d ! Includes fit to moments, van Hees et al, ! Nucl. Phys. A476, 61 (1988) and pri. comm. p pjp a e ! JULIES-RICHTER POT INT p pjt a f ! JULIES-RICHTER TBME INT ! S. Afr. Tydskr.Fis. 15 nr. 3/4 (1992) p mp a g ! D.J.MILLENER (PRIVATE COMMUNICATION NOV 1984) p pewt a h ! * P(10-16)T: WARBURTON A=10-16 TBME INT (1991) p pwt a i ! * P(5-16)T: WARBURTON A= 5-16 TBME INT (1991) p pkuo a j ! * Kuo, Paris interaction, Private Comm. (1989) p psu3 a k ! * SU3 INT - OCT 1990 VERSION p ckihe a l ! * CKI plus fit to He isotopes PRC37, 2220 (1988). ! ---------------------------------------------- ! ---------------------------------------------- ! PPN Model Space ! P1p1/2,P1p3/2,N1p1/2,N1p3/2 orbits ppn ckppn a 1 ! (8-16)POT S. Cohen and D. Kurath, ppn ckipn a 2 ! (6-16)TBME Nucl. Phys. A73, 1 (1965) and ppn ckiipn a 3 ! (8-16)TBME Nucl. Phys. A101, 1 (1967) ppn pmompn a 4 ! Includes fit to moments, van Hees et al, ! Nucl. Phys. A476, 61 (1988) and pri. comm. ppn pjppn a 5 ! * JULIES-RICHTER POT INT (1988) ppn pjtpn a 6 ! * JULIES-RICHTER TBME INT (1988) ppn su3ppn a 7 ! SU3 INT ! ---------------------------------------------- ! ORMAND-BROWN INC, NPA491, 1 (1989) ! original int + PCOSPN + CKPIVPN + CKPITPN ! ppn ckpcdpn a u ! (8-16)POT S. Cohen and D. Kurath, ppn ckicdpn a v ! (6-16)TBME Nucl. Phys. A73, 1 (1965) and ppn ckiicdpna w ! (8-16)TBME Nucl. Phys. A101, 1 (1967) ppn pjpcdpn a x ! * JULIES-RICHTER POT INT (1988) ppn pjtcdpn a y ! * JULIES-RICHTER TBME INT (1988) ppn pmomcdpna z ! Includes fit to moments, van Hees et al, ! ---------------------------------------------- ! ---------------------------------------------- ! SD Model Space ! 1d3/2,1d5/2,2s1/2 orbits sd sdba b k ! * BONN A FROM Hjorth-Jensen, SEP 2000 sd kuosd b e ! RENORMALIZED KUO NPA103, 71 (1967) sd kuosdm b y ! " " PLUS (A/18)**0.3 MASS DEPENDENCE sd bkuosd b k ! BARE KUO NPA103, 71 (1967) sd pw b d ! (PW) PREEDOM-WILDENTHAL PR C6, 1633 (1972) sd cw b c ! (CW) CHUNG-WILDENTHAL A=17-28 INTERACTION sd cwh b h ! (CW) CHUNG-WILDENTHAL A=28-39 INTERACTION sd kuosdh b g ! K12.5P from Chung's thesis sd sdm b m ! WILDENTHAL-MCGRORY MSDI (PRC4, 1708 (1971)) sd w b w ! (W) WILDENTHAL'S A=17-39 "USD" INT (JULY 1982) sd usda b a ! Phys. Rev. C74, 034313 (2006) sd usdb b b ! Phys. Rev. C74, 034313 (2006) sd hbusd b j ! SDPOTA int from Ann. Phys. 182, 191 (1988) sd hbumsd b i ! SDPOTB int from Ann. Phys. 182, 191 (1988) sd su3sd b s ! SU3 INT - OCT 1990 VERSION ! ---------------------------------------------- ! ---------------------------------------------- ! SDPN Model Space ! P0d3/2,P0d5/2,P1s1/2,N0d3/2,N0d5/2,N1s1/2 orbits sdpn usdapn b 1 ! usda in pn sdpn usdbpn b 2 ! usdb in pn sdpn wpn b 3 ! "USD" INT PN FORMALSIM sdpn wcpn b 4 ! "USD" INT PN FORMALSIM plus Coulomb sdpn wcdpn b 5 ! "USD" PLUS COULOMB PLUS "USD" ISOVECTOR AND ! ISOTENSOR, NPA491, 1 (1989) sdpn usdbcdpnb x ! "usdb" PLUS COULOMB PLUS "USD" ISOVECTOR AND sdpn cwhcdpn b v ! "CWH" PLUS COULOMB PLUS "USD" ISOVECTOR AND ! ISOTENSOR, NPA491, 1 (1989) sdpn sdmpn b v ! MSDI (PRC4, 1708 (1971)) IN PN FORMALISM sdpn sdmcdpn b v ! MSDI (PRC4, 1708 (1971)) PLUS INC INTERACTION ! OF TOWNER & HARDY (NPA205, 33 (1973)) ! SHSP.FOR(SDMCDPN = SDMPN+SDMTEN) sdpn wcdnp b u ! SAME AS WCDPN EXCEPT P-N LABELS INTERCHANGED sdpn wwcdnp b u ! SAME AS WWCDPN EXCEPT P-N LABELS INTERCHANGED sdpn sdmcdnp b v ! SAME AS MCDPN EXCEPT P-N LABELS INTERCHANGED ! SHSP.FOR(SDMCDNP = SDMNP+SDMTEN) sdpn su3sdpn b t ! SU3 INT ! ---------------------------------------------- ! ---------------------------------------------- ! ZBM Model Space ! 1p1/2,1d5/2,2s1/2 orbits zbm zbmi c a ! (I) ZUKER-BUCK-MCGRORY PRL 21, 39 (1968) zbm zbmii c b ! (II) ZUKER-BUCK-MCGRORY PRL 21, 39 (1968) zbm rewil c r ! MCGRORY-WILDENTHAL PRC7, 974 (1973) (F-INT) FROM ! REEHAL-WILDENTHAL PART AND NUCL 6, 137 (1973) zbm zwm c z ! MCGRORY-WILDENTHAL PRC7, 974 (1973) (Z-INT) FROM ! ZUKER PRL 23, 983 (1969) zbm su3zbm c s ! SU3 INT ! ---------------------------------------------- ! ---------------------------------------------- ! ZBME Model Space ! 1p1/2,1d5/2,2s1/2,d3/2 orbits zbme rewile c q ! REEHAL-WILDENTHAL PART AND NUCL 6, 137 (1973) ! F-INT IN PRC7, 974 (1973) zbme zwme c y ! MCGRORY-WILDENTHAL PR C7, 974 (1973) (Z-INT) zbme su3zbme c t ! SU3 INT ! ---------------------------------------------- ! ---------------------------------------------- ! ZBMPN Model Space ! P1p1/2,P1d5/2,P2s1/2,N1p1/2,N1d5/2,N2s1/2 orbits zbmpn rewilpn c p ! REEHAL-WILDENTHAL PART AND NUCL 6, 137 (1973) zbmpn zbmipn c e ! REWILPN + INC INTERACTION, AUG 1987 zbmpn zbmiipn c f ! REWILPN + INC INTERACTION, AUG 1987 zbmpn rwcdpn c c ! REWILPN + INC INTERACTION, AUG 1987 ! ---------------------------------------------- ! ---------------------------------------------- ! PSD Model Space ! 1p1/2,1p3/2,1d3/2,1d5/2,2s1/2 orbits ! SHELL will include the center of mass ! Hamiltonian PSDCM in the list of inputs ! to MATRIX psd psdwbt d a ! EKW-BAB LC48 TBME FIT; PSDT+PSDW, 40 2HW TBME from WBP psd psdwbp d b ! EKW-BAB POTENTIAL FIT; PSDP+PSDW, 40 2HW TBME from WBP psd psdmk d d ! MK(P-SD) + PW(SD) + CKPOT(P) psd psdmwk d e ! MK(P-SD) + W(SD) + MP(P) psd psdvh d f ! van Hees's psd interaction (via F. Barker) psd psdsu3 d h ! SU3 INT ! ---------------------------------------------- ! ---------------------------------------------- ! PSDPN Model Space ! P 1p1/2,1p3/2,1d3/2,1d5/2,2s1/2 orbits ! N 1p1/2,1p3/2,1d3/2,1d5/2,2s1/2 orbits ! SHELL will include the center of mass ! Hamiltonian PSDCMPN in the list of inputs ! to MATRIX psdpn psdmwkpnd u ! MP(P) + W(SD) + MK(OTHER) ! ---------------------------------------------- ! ---------------------------------------------- ! SPSDPF Model Space ! 1s1/2,1p3/2,1p1/2,1d5/2,1d3/2,2s1/2 ! 1f7/2,1F5/2,2P3/2,2P1/2 orbits ! SHELL will include the center of mass ! Hamiltonian SPSDPFCM in the list of inputs ! to MATRIX spsdpf spfsu3 t s ! SU3 spsdpf wbt t t ! SPSDPFT +SPSDPFMW+0S0F1P0(H7B;OTHERS), MAR 1992 spsdpf wbp t p ! SPSDPFPB(2HW:WBP)+SPSDPFMW+0S0F1P0(H7B;OTHERS) spsdpf wbn t n ! EKW-BAB POTENTIAL FIT; PSDP+PSDW, 40 2HW TBME from WBP n5 wbp 5 p ! SPSDPFPB(2HW:WBP)+SPSDPFMW+0S0F1P0(H7B;OTHERS) spsdpf wbb t b ! same as WBP but w.int replaced by USDB.int ! plus spsdpfbn.int(p-sd,off-diagonal) spsdpf wbm t m ! WBP WITH USD*X ! WB* interactions listed above are via ! E. K. Warburton and B. A. Brown, Phys. Rev. C ! 46, 923 (1992). ! ---------------------------------------------- ! ---------------------------------------------- ! D3F7 Model Space ! 1d3/2,1f7/2 orbits d3f7 w0 g s ! WILDENTHAL AS USED IN PRL 33, 233 (1974) d3f7 sas g a ! SAKAKURA-ARIMA-SEBE PL 61B, 335(1976) d3f7 fep g f ! FEDERMAN-PITTEL PR 186, 1106 (1969) d3f7 hw g h ! S.T.Hsieh, X.Ji, R.Mooy and B.H.Wildenthal in ! "Nuclear Structure at High Spin, Excitation ! and Momentum Transfer", edited by H. Nann, ! AIP Conference Proceedings 142, (American ! Institue of Physics, 1986), p. 357. ! ---------------------------------------------- ! ---------------------------------------------- ! D3F7PN Model Space ! P1d3/2,P1f7/2,N1d3/2,N1f7/2 orbits ! (SEE SUBROUTINE PN_INT FOR RELABELING OF *.MAT ! *.EIG, *.LPE AND *.GND FILES) d3f7pn saspn g b ! SAS INT PN FORMALSIM d3f7pn hwpn g u ! * "HW" INT PN FORMALSIM d3f7pn hwcdpn g u ! * "HW" PLUS COULOMB PLUS "HW" ISOTENSOR d3f7pn hwcdnp g u ! * SAME AS HWCDPN EXCEPT P-N LABELS INTERCHANGED ! ---------------------------------------------- ! ---------------------------------------------- ! HASP Model Space ! 1d3/2,2s1/2,2p3/2,1f7/2 orbits hasp hasp g i ! + parity int from HASPER, PRC19, 1482 (1979) hasp hasn g j ! - parity int from HASPER, PRC19, 1482 (1979) hasp vpnp g k ! MSDI int: van-der-Poel Nucl. Phys. A373, 81 (82) hasp vpth g l ! MSDI int: van-der-Poel Thesis, p.50 (JAB) ! ---------------------------------------------- ! ---------------------------------------------- ! SDPF Model Space ! * 1d5/2,1d3/2,2s1/2,1f7/2,1f5/2,2p3/2,2p1/2 sdpf sdpfm40 l i ! Phys. Rev. C34, 1031 (1986) ! SHSP.FOR(SDPFM40 = SDPFW + SDPFVHB + SDPFM40) ! (SDPF)VHB = PFVH + (F7/2)**2 MADE TO FIT 42SC ! (SDPF)M40 = MILLENER-KURATH D3-F7 EXACT FIT ! TO 1P1H STATES IN 40CA EXCEPT FOR 3- T=0 sdpf sdpfmw l h ! Phys. Rev. C41, 1147 (1990) (better than M40) ! called WBMB in BNL Report 40890(1987) ! SHSP.FOR(SDPFMW = SDPFW + SDPFMC + SDPFMW) ! (SDPF)W = (SD)W FOR A=40 ! (SDPF)MC = MCGRORY; PHYS.REV. C8, 693(1973) ! (SDPF)MW = (SDPF)M40 EXCEPT SPE CHANGED TO ! GIVE MCGRORY'S FP VALUES. sdpf sdpfwb l w ! SHSP.FOR(SDPFWB = SDPFW + SDPFMC + SDPFWB) ! (SDPF)W = (SD)W FOR A=40 ! (SDPF)MC = MCGRORY; PHYS.REV. C8, 693(1973) ! (SDPF)WB = MODIFIED SDPFMW ! See p29 of BNL Report 40890(1987). The MK ! potential (overall) strength was increased ! by 20% and some other changes were made in ! it as noted the the (amended) report. sdpf sdpfwa l m ! (1990) Works better around A=48 than SDPFMW ! SHSP.FOR(SHPFWA = SDPFW + SDPFBP + SDPFMK) ! (SDPF)W = (SD)W FOR A=40 ! (SDPF)BP = (FP)BP ! (SDPF)MW = MILLENER-KURATH sdpf sdpfnow l n ! SDPF INTERACTION (from PRC 63 (2001) 44316) ! ---------------------------------------------- ! * SDPFPN Model Space ! * P1d5/2,1d3/2,2s1/2,1f7/2,1f5/2,2p3/2,2p1/2 ! * N1d5/2,1d3/2,2s1/2,1f7/2,1f5/2,2p3/2,2p1/2 sdpfpn nowpn l p ! pn version of sdpfnow ! ---------------------------------------------- sdpfpn sdpfmwpnl g ! * SHSP.FOR(SDPFMWPN=SDPFWPN+SDPFMCPN+SDPFMWPN) ! (SDPF)W = (SD)W FOR A=40 ! (SDPF)MC = MCGRORY; PHYS.REV. C8, 693(1973) ! (SDPF)MW = (SDPF)M40 EXCEPT SPE CHANGED TO ! GIVE MCGRORY'S FP VALUES. ! ---------------------------------------------- ! ---------------------------------------------- ! F7 Model Space ! 1f7/2 orbits f7 f7mbz e m ! J. D. McCullen, B. F. Bayman and L. Zamick ! Phys. Rev. 134, B515 (1963). f7 f742 e a ! KUTCHERA et al. "42SC" R NUOVO CIM, VOL-1 NO-12 f7 f748 e b ! KUTCHERA et al. "48SC" R NUOVO CIM, VOL-1 NO-12 f7 f754 e c ! KUTCHERA et al. "54CO" R NUOVO CIM, VOL-1 NO-12 ! ---------------------------------------------- ! ---------------------------------------------- ! F7PN Model Space ! P1f7/2,N1f7/2 orbits f7pn f742pn e u ! KUTCHERA PN INT BASED ON 42TI, 42SC AND 42CA f7pn f748pn e v ! KUTCHERA PN INT BASED ON 50TI, 48SC AND 50TI f7pn f748bpn e w ! KUTCHERA PN INT BASED ON 50TI, 48SC AND 46CA f7pn f7cdpn e s ! Brown and Sherr, NPA322, 61 (1979) ! ---------------------------------------------- ! ---------------------------------------------- ! FP Model Space ! 1f7/2,2p3/2,1f5/2,2p1/2 orbits fp su3fp f s ! SU3 INT - OCT 1990 VERSION fp gx1 f 1 ! GXFP1 fp gx2 f 2 ! GXFP2 fp kb3 f 3 ! KB3 fp kb3g f 4 ! KB3G fp gx1a f 5 ! GXFP1A fp kbf f 6 ! KBF fp fpd6 f o ! Richter et al., Nucl. Phys. A523, 325 (1991) ! FULL FP POTENTIAL FIT - AUG 1989 ! called FPD6 in Table 7 of this paper fp fpbm f r ! Richter et al., Nucl. Phys. A523, 325 (1991) ! FULL FP TBME FIT - AUG 1989 ! called FPMI3 in Table 7 of this paper fp fpd6n f n ! FPBP WITH SPE ADJUSTED FOR 56NI fp fpm f m ! MOOY INTERACTION ! ZP A312, 59 (1983) AND PRIVATE COMMUNICATION fp fpy f y ! F7P3F5P1 + YOKOYAMA "D" INTERACTION ! PHYS REV C31, 1012 (1985) AND PRIV COMM ! PLUS MSDI(0.25,0.53,-1.09,.50) ! FOR ALL OTHER MATRIX ELEMENTS FROM THE ! 1ST COLUMN IN TABLE 1 OF ! KOOPS AND GLAUDEMANS, Z. PHYS. A280, 181 (1977) fp fpv f v ! VAN HEES INTERACTION Z. PHYS. A303, 267 (1981) ! PLUS MSDI(0.25,0.53,-1.09,.50) ! FOR ALL OTHER MATRIX ELEMENTS FROM THE ! 1ST COLUMN IN TABLE 1 OF ! KOOPS AND GLAUDEMANS, Z. PHYS. A280, 181 (1977) fp fpvh f h ! SAME AS FPV BUT REPLACING F5P1P3 WITH ! WITH VAN HIENEN - CHUNG - WILDENTHAL ! INTERACTION NPA269, 159 (1976) fp fpv2 f t ! FPV + 2 MEV ADDED ONTO F5/2 ORBIT ! TO GET BETTER 1+ PH SPECTRUM IN 48CA ! SEE B.D.ANDERSON ET AL, PRC31, 1161 (1985) fp fprkb f k ! RENORMALIZED KUO-BROWN, NPA114, 241 (1986) fp fpbkb f l ! BARE KUO-BROWN, NPA114, 241 (1986) ! fp fpmcc f x ! FPRKB + 15 TBME CHANGED BY ! J.B.McGrory, B. H. Wildenthal and E.C.Halbert ! Phys. Rev. C2, 186 (1970) fp fpmcd f x ! FPRKB + 8 TBME CHANGED FOR |F7/2,F7/2,J,T> ! AND NEW S.P.E. ! F7/2=-8.36, P3/2=-6.26, F5/2=-1.86, P1/2=-4.46 ! J.B.McGrory, Phys. Rev. C8, 693 (1973) fp fpmce f x ! FPMCC + 50 KeV CHANGED TO F7-F5 + NEW S.P.E. ! 0.0(1F7/2), 2.1(2P3/2), 4.4(2P1/2), 8.2(1F5/2) ! J.B.McGrory and B.H.Wildenthal, ! Phys. Lett. 103B, 173 (1981) fp fpmh f f ! FPMCE + SHIFT THE MONOPOLE OF INTER-SHELL ! INTERRACTION (J,T=0) BY -0.3 MeV ! K.Muto and H.Horie, Phys.Lett. 138B, 9 (1984) ! --------------------------------------------- ! ---------------------------------------------- ! FPPN Model Space ! P1f7/2,2p3/2,1f5/2,2p1/2 orbits ! N1f7/2,2p3/2,1f5/2,2p1/2 orbits ! (SEE SUBROUTINE PN_INT FOR RELABELING OF *.MAT ! * fppn gx1pn f a ! GXFP1 IN PN fppn gx2pn f b ! GXFP2 IN PN fppn kb3pn f c ! KB3 IN PN fppn kb3gpn f d ! KB3G IN PN fppn gx1apn f e ! gxpf1a in pn fppn fpd6pn f y ! "FPD6" INT PN FORMALSIM fppn fpd6npn f x ! "FPD6N" INT PN FORMALSIM fppn fpd6cdpnf z ! "FPD6" PLUS COULOMB PLUS "FPD6" ISOTENSOR fppn fpd6cdnpf z ! SAME AS FPBCDPN EXCEPT P-N LABELS INTERCHANGED fppn fpvpn f u ! "FPV" INT PN FORMALSIM fppn fpvcdpn f u ! "FPV" PLUS COULOMB PLUS "FPV" ISOTENSOR fppn fpvcdnp f u ! SAME AS FPVCDPN EXCEPT P-N LABELS INTERCHANGED ! --------------------------------------------- ! --------------------------------------------- ! HO Model Space ! P1f7/2,N2p3/2,N15f/2,N2p1/2 orbits ho ho h h ! H.Horie and K.Ogawa, Prog. of Theoretical ! Physics 46, 439 (1971), Nucl. Phys. A216, ! 407 (1973). ! --------------------------------------------- ! ---------------------------------------------- ! F5P Model Space ! 1f5/2,2p3/2,2p1/2 orbits f5p f5pvh h w ! WITH VAN HIENEN - CHUNG - WILDENTHAL ! INTERACTION NPA269, 159 (1976) ! --------------------------------------------- ! ---------------------------------------------- ! GL Model Space ! P2p1/2,P1g9/2,N3s1/2,N2d5/2 orbits gl gl i g ! GLOECKNER INTERACTION (FINAL) NPA253, 301 (1975) gl glb i h ! GLOECKNER INTERACTION, BARE G-MATRIX(N=51) ! ---------------------------------------------- ! ---------------------------------------------- ! N50J Model Space ! 2P3/2,1F5/2,2p1/2,1g9/2 n50j n50j i j ! JI-WILDENTHAL INTERACTION (N=50) ! ---------------------------------------------- ! jj44 model space ! proton f5/2,p3/2,p1/2,g9/2 jj44 jj44b i b ! f4.int 4th iteration for A=56-100 fit ! Brown and Lisetskiy, unpublished ! ---------------------------------------------- ! jj4pn model space ! proton f5/2,p3/2,p1/2,g9/2 ! neutron f5/2,p3/2,p1/2,g9/2 jj44pn jj44pna i a ! T=1 interactions only from PRC70, 044314 (2004) jj44pn jj44bpn i 2 ! pn version of jj44b ! ---------------------------------------------- ! --------------------------------------------- ! GLEPN Model Space ! P2P3/2,1F5/2,2p1/2,1g9/2,3s1/2,2d5/2,2D3/2 ! N2P3/2,1F5/2,2p1/2,1g9/2,3s1/2,2d5/2,2D3/2 glepn glepn i m ! H. Mach et al., PRC41, 226 (1990) glepn glbepn i i ! H. Mach et al., PRC41, 226 (1990) ! --------------------------------------------- ! ---------------------------------------------- ! GLEKPN Model Space ! P1F7/2,1F5/2,2P3/2,2P1/2,1G9/2 ! N1G9/2,1G7/2,2D5/2,2D3/2,3S1/2 glekpn glekpn i k ! H. Mach et al., PRC41, 226 (1990) ! --------------------------------------------- ! ---------------------------------------------- ! SLG Model Space ! P2p1/2,P1g9/2,N2p1/2,N1g9/2 orbits slg slgm j a ! "seniority-fit total-energy" PP and PN SLG int ! F.J.D.Serduke, R.D.Lawson and D.H.Gloeckner ! NPA256, 45 (1976) ! * NN INTERACTION FROM BAB slg slgmt0 j z ! "T=0" PP and PN SLG int ! * NN INTERACTION FROM BAB slg slgml j l ! "seniority-fit levels" PP and PN SLG int ! * NN INTERACTION FROM BAB slg slgo j b ! PP AND PN SERDUKE-LAWSON-GLOECKNER INTERACTION ! * NN INTERACTION FROM ZP314, 205 (1983) ! (LAWSON PRIVATE COMMUNICATION) slg slgtpn j s ! SLGT INTERACTION slg slgt0pn j z ! SLGT0 Herndl-Brown - NPA627, 35 (1997) slg slgj j j ! PP AND PN SERDUKE-LAWSON-GLOECKNER INTERACTION ! * NN INTERACTION FROM BAB & THE PP TBME FROM ! JI & WILDENTHAL. ! ---------------------------------------------- ! --------------------------------------------- ! SLGT Model Space ! 2p1/2,1g9/2 slgt slgt j t ! SPACE SERDUKE-LAWSON-GLOECKNER INTERACTION slgt slgt0 j w ! Herndl-Brown - NPA627, 35 (1997) ! --------------------------------------------- ! SN Model Space ! P1F5/2,2P3/2,2p1/2,1G9/2,1G7/2,2d5/2,2D3/2,3S1/2 ! N1F5/2,2P3/2,2p1/2,1G9/2,1G7/2,2d5/2,2D3/2,3S1/2 sn snt i t ! ! SNT Model Space ! P1F5/2,2P3/2,2p1/2,1G9/2,1G7/2,2d5/2,2D3/2,3S1/2 ! N1F5/2,2P3/2,2p1/2,1G9/2,1G7/2,2d5/2,2D3/2,3S1/2 ! N1H11/2 sne snet i v ! ! ---------------------------------------------- ! N82 Model Space ! P - 1G7/2,2D5/2,2D3/2,3S1/2,1H11/2 n82 n82k m k ! Kruse-Wildenthal, BAPS 27, 533 (1982) p. 725. n82 n82a m a ! Bonn-A from Horjth-Jensen n82 n82b m b ! Bonn-B from Horjth-Jensen n82 n82c m c ! CD-Bonn from Horjth-Jensen n82 n82d m d ! Nijmegen I from Horjth-Jensen ! ---------------------------------------------- ! ---------------------------------------------- ! jj45pn Model Space ! P - 2P1/2,2P3/2,2F5/2,1G9/2 ! N - 1G7/2,2D5/2,2D3/2,3S1/2,1H11/2 jj45pn jj45pna r g ! G matrix for 132Sn from Horth-Jensen (2000) ! with spe adjusted to 132Sn region ! ---------------------------------------------- ! ---------------------------------------------- ! jj55pn model space ! P - 1G7/2,2D5/2,2D3/2,3S1/2,1H11/2 ! N - 1G7/2,2D5/2,2D3/2,3S1/2,1H11/2 jj55pn sn100pn q g ! Phys. Rev. C 71, 044317 (2005) ! --------------------------------------------- ! ---------------------------------------------- ! jj56pn model space ! P=1G7/2,2D5/2,2D3/2,3S1/2,1H11/2 ! N=1H9/2,2F7/2,2F5/2,3P3/2,3P1/2,1I13/2 ! ---------------------------------------------- jj56pn kh5082 u p ! KHH(PURE)*(208/132)**(1/3), for a A=132 CORE ! RATHER THAN 208; EXPT. SPE ! W.T.Chou and E.K.Warburton, PRC45, 1720 (1992). jj56pn cw5082 u w ! Z50n82 but with the pp tbme and the p spe replaced ! by the N82K values. ! W.T.Chou and E.K.Warburton, PRC45, 1720 (1992). jj56pn cwg u g ! Phys. Rev. C 71, 044317 (2005) ! --------------------------------------------- ! --------------------------------------------- ! PB206 model space ! N (holes) 0H9,1F7,1F5,2P3,1P1,0I13 pb206 pb206ba w a ! THE KUO-HERLING BARE TBME pb206 pb206bu w b ! THE KUO-HERLING 1P-1H BUBBLE pb206 pb206mc w c ! G(bare)+0.75*G(cp), McGrory and Kuo, ! NPA247, 283 (1975). NOTE: Blomqvist-McGrory ! changed quite a few TBME to tune to 206Pb. pb206 pb206jb w d ! G(bare)+0.75*G(cp), McGrory and Kuo, ! NPA247, 283 (1975). NOTE: Blomqvist-McGrory ! changed quite a few TBME to tune to 206Pb. ! Other changes have been made- ! see heading of .int file. ! This is the preferred interaction in this space. pb206 pb206wm w e ! MSDI, D. Wang and M. T. McEllistrem, ! Phys. Rev. C42, 252 (1990) pb206 pb206bm w g ! THE KH-MC BARE; PB206JB - 0.75*PB206BU ! ---------------------------------------------- ! ---------------------------------------------- ! jj45pn (KHH) model space ! P=1G7/2,2D5/2,2D3/2,3S1/2,1H11/2 ! N=1H9/2,2F7/2,2F5/2,3P3/2,3P1/2,1I13/2 ! NOTE for the kh interactions that the number of ! "particles" is the number of holes relative to 208Pb jj56pn khhba v a ! KUO-HERLING: McGrory&Kuo, N.P. A247, 283 (1975). ! THE 'BARE' G-MATRIX OF KUO&HERLING. jj56pn khhbu v b ! KUO-HERLING: McGrory&Kuo, N.P. A247, 283 (1975). ! THE 1P1H 'BUBBLE' OF KUO&HERLING. jj56pn khh v c ! PHYS. REV. C 43 (1991) 602. ADAPTED FROM ! KUO-HERLING: McGrory&Kuo, N.P. A247, 283 (1975). ! SEE ALSO Phys. Rev. C 24, 717 (1981). ! THE HOLE SPACE (BELOW 208PB), KHHBA+KPH*KHHBU: ! KPH(PP)=0.70,KPH(PN)=0.75,KPH(NN)=0.55 ! ---------------------------------------------- jj56pn khhe v d ! THIS IS THE PREFERRED INTERACTION FOR THIS SPACE. ! PHYS. REV. C 43 (1991) 602. ADAPTED FROM ! KUO-HERLING: McGrory&Kuo, N.P. A247, 283 (1975). ! SEE ALSO Phys. Rev. C 24, 717 (1981). ! THE HOLE SPACE (BELOW 208PB), BARE+1.00*BUBBLE ! FOR PP & PN [&SELECTED TBME TUNED TO 206TL & ! 206HG AS PER NUCL.PHYS.A512, 217 (1990)], ! PB206JB FOR NN. ! ---------------------------------------------- ! ---------------------------------------------- ! jj67pn (KHP) model space ! P=1H9/2,2F7/2,2F5/2,3P3/2,3P1/2,1I13/2 ! N=1I11/2,2G9/2,2G7/2,3D5/2,3D3/2,4S1/2,1J15/2 jj67pn khpba v o ! KUO-HERLING: McGrory&Kuo, N.P. A247, 283 (1975). ! THE 'BARE' G-MATRIX OF KUO&HERLING. jj67pn khpbu v i ! KUO-HERLING: McGrory&Kuo, N.P. A247, 283 (1975). ! THE 1P1H 'BUBBLE' OF KUO&HERLING. jj67pn khp v e ! PHYS. REV. C 43 (1991) 602. ADAPTED FROM ! KUO-HERLING: McGrory&Kuo, N.P. A247, 283 (1975). ! SEE ALSO PHYS. Rev. C 24, 717 (1981). ! THE PARTICLE SPACE (ABOVE 208PB), ! KHPBA+KPH*KHPBU ! KPH(PP)=0.92,KPH(PN)=0.90,KPH(NN)=1.07 ! ---------------------------------------------- jj67pn khpe v f ! THIS IS THE PREFERRED INTERACTION FOR THIS SPACE. ! PHYS. REV. C 43 (1991) 602. ADAPTED FROM ! KUO-HERLING: McGrory&Kuo, N.P. A247, 283 (1975). ! SEE ALSO PHYS. Rev. C 24, 717 (1981). ! THE PARTICLE SPACE (ABOVE 208PB), ! KHPBA+KPH*KHPBU ! KPH(PP)=0.92,KPH(PN)=0.90,KPH(NN)=1.07 ! & MANY PNP TBME ADJUSTED. THE CHANGED PNP TBME ! ARE LABELED AS SUCH. 'E' IS FOR EMPIRICAL. ! +49 AND +15 KeV HAS BEEN ADDED TO THE DIAGONAL ! PP AND NN TBME, RESPT. ! ---------------------------------------------- ! PBPOP model space ! P=2D5/2,2D3/2,3S1/2,0H11/2,0H9/2,1F7/2,0I13/2 ! N=2F5/2,3P3/2,3P1/2,0113/2,1G9/2,0I11/2,0J15/2 pbpop pbpop v s ! Poppelier&Glaudemans, Z.Phys.A 329 (1988) 275 ! 1P-1H INTERACTION ! ---------------------------------------------- ! 24 j states, 178 m states. A cm int. - PBACM also pb208 pb208g v g ! end !