56V ADOPTED LEVELS ENSDF 202203 56V H TYP=FUL$AUT=Balraj Singh$CIT=ENSDF$CUT=25-Mar-2022 56V H TYP=FUL$AUT=HUO JUNDE, HUO SU, YANG DONG$CIT=NDS 112, 1513 (2011)$ 56V 2 H CUT=29-Oct-2009$ 56V Q 910E1 18 513E1 18 1164E1 18 -808E1 18 2021WA16 56V cQ $Q(|b{+-}n)=860 {I180}, S(2n)=12430 {I180}, S(2p)=26320 {I180} 56V 2cQ (2021Wa16) 56V c 1990Tu01, 1994Se12: {+56}V produced in proton-induced fragmentation 56V 2c and fission reactions on natural Thorium using the high-intensity 56V 3c proton beam of the Los Alamos Meson Physics Facility. Measured mass 56V 4c excess of g.s. of {+56}V using Time-of-Flight Isochronous (TOFI) 56V 5c spectrometer. 56V c 1996Do23: {+56}V produced in the decay of {+56}Ti. Measured 56V 2c |b|g-coin activity 56V c 1998So03: {+56}V produced in {+9}Be({+65}Cu,X) at 56V 2c E({+65}Cu=64.5 MeV/nucleon and separated by LISE spectrometer at GANIL. 56V 3c Measured |b|g-coin, and T{-1/2} of {+56}V decay 56V d 1995ZoZX and 1996SoZY superseded by 1998So03 56V c 1998Am04 (also 1997AmZZ thesis): {+56}V produced and identified in 56V 2c the fragmentation of 500 MeV/nucleon {+86}Kr beam with 2 g/cm{+2} 56V 3c {+9}Be target and separation of fragments using FRS spectrometer at 56V 4c GSI facility. Measured (implants)|b-correlations, and T{-1/2} of 56V 5c decay of {+56}V 56V d 1995AmZX and 1995AmZY superseded by 1998Am04. 56V c 2003Ma02: {+56}V produced in {+9}Be({+86}Kr{+34+},X) 56V 2c at E=140 MeV/nucleon, followed by separation of fragments using A1900 56V 3c fragment separator at NSCL-MSU. Measured E|g, I|g, |g|g-coin, 56V 4c |b|g-coin, T{-1/2} of {+56}V decay using a double-sided 56V 5c Si microstrip detector (DSSD) and Segmented Germanium Array (SeGA) 56V 6c arranged around the |b counting system. 56V c 2015Al19: yield measurement in {+2}H({+136}Xe,X),E=500 MeV/nucleon, 56V 2c with residues analyzed using the FRS magnetic spectrometer and 56V 3c multisampling ionization chambers at GSI facility 56V c Mass measurements: 1994Se12 (also 1995ViZX), 1990Tu01. 56V c Theoretical calculations: six primary reference extracted from the NSR 56V 2c database (www.nndc.bnl.gov/nsr/), listed here under document records. 56V d Theory references: 2021Ra26, 2019Li23, 2018Sa40, 2016Ku21, 2012Ch48, 56V 2d 2001La24 56V XA56TI B- DECAY (200 MS) 56V L 0.0 1+ 216 MS 4 56V 2 L %B-=100 $ %B-N=? 56V X L XREF=A$ 56V cL $Theoretical T{-1/2}=0.297 s, %|b{+-}n=0 (2019Mo01). 56V cL $Theoretical T{-1/2}=6.6 s, %|b{+-}n=0 (2021Mi17). 56V cL T$from 2003Ma02 (fragment-|b and fragment-|b-|g correlated decay 56V 2cL curves). Others: 0.24 s {I4} (1998Am04, implants-|b correlated 56V 3cL decay curves); 230 ms {I25} (1998So03, singles-|b and |b|g-coin decay 56V 4cL curves) are in agreement with value from 2003Ma02, but 56V 5cL much less precise. 56V cL J$log| {Ift}=4.62 to 0+ ground state of {+56}Cr 56V cL $Proposed configuration=|p3/2[321]~#|n3/2[312] (1998So03), with 56V 2cL 1+ assignment for the g.s. of {+56}V 56V COMMENTS ENSDF 202203 56V H TYP=FUL$AUT=Balraj Singh$CIT=ENSDF$CUT=25-Mar-2022 56V C TITL$NUCLEAR DATA SHEETS FOR 56V 56V c AUTH$BALRAJ SINGH 56V c INST$Department of Physics and Astronomy 56V #c McMaster University, Hamilton, ON L8S 4M1, Canada 56V c ABST$Nuclear Structure data for {+56}V has been evaluated, which 56V 2c supersede that in the previous evaluation published by 2011Hu08 and in 56V 3c the ENSDF database 56V c CUT$All literature available up to March 25, 2022 has been considered. 56V C CIT$ENSDF 56V 56TI B- DECAY (200 MS) 2003MA56,1998AM04,1996DO23ENSDF 202203 56V H TYP=FUL$AUT=Balraj Singh$CIT=ENSDF$CUT=25-Mar-2022 56V H TYP=FUL$AUT=HUO JUNDE, HUO SU, YANG DONG$CIT=NDS 112, 1513 (2011)$ 56V 2 H CUT=29-Oct-2009$ 56V c 2003Ma56: {+56}Ti isotope produced in {+9}Be({+86}Kr{+34+},X) at 56V 2c E({+86}Kr)=140 MeV/nucleon followed by separation of fragments using 56V 3c A1900 fragment separator. Measured E|g, I|g, |g|g-coin, |b|g-coin, 56V 4c T{-1/2} using a double-sided Si microstrip detector (DSSD) 56V 5c and Segmented Germanium Array (SeGA) arranged around the |b 56V 6c counting system. 56V c 1998Am04: {+56}Ti isotope produced in {+9}Be({+86}Kr{+34+},X) at 56V 2c E({+86}Kr)=500 MeV/nucleon, fragments separated using FRS fragment 56V 3c separator at GSI by a combination of B|r, |DE and tof techniques. 56V 4c Measured T{-1/2} of decay of {+56}Ti 56V c 1996Do23: {+56}Ti isotope produced in {+9}Be({+65}Cu{+26+},X) 56V 2c at E=64.5 MeV/nucleon; identification of particle from energy loss 56V 3c and tof at GANIL. Measured singles |b{+-} and |b|g-coin. 56TI P 0.0 0+ 200 MS 5 676E1 19 56TI cP T$From {+56}Ti Adopted Levels 56TI cP QP$From 2021Wa16 56V N 1.0 1.0 56V L 0.0 1+ 216 MS 4 56V cL J,T$from the Adopted Levels 56V B 94 3 3.86 6 56V S B EAV=3124 93 56V cB IB$no evidence was found by 2003Ma56 for delayed g rays from {+56}Ti 56V 2cB decay with absolute |g-ray intensity greater than 2%. Further search 56V 3cB for |g rays in {+55}V for possible |b-delayed neutron decay mode of 56V 4cB {+56}Ti did not show any |g rays. On this basis, 2003Ma56 deduced |b 56V 5cB branching of 94% {I3} to {+56}V ground state, with little or no 56V 6cB |b branching to excited states in {+56}V. 56V 7cB $ Note that results in 1996Do23 are in contradiction to those from 56V 8cB 2003Ma56. 1996Do23 estimated that 40% of all the {+56}Ti |b decay to 56V 9cB low-lying levels in {+56}V in the range of 0.2 MeV to 0.8 MeV from a 56V AcB comparison of the numbers of {+56}Ti |b singles and |b|g-coin events, 56V BcB while excluding |b feeding of the g.s. of {+56}V, as also in the 56V CcB decay of {+54}Ti decay.