14B 17B(1H,1H3NG):XUNDL-1 2005KA06 200507 14B c BEAM={+17}B, TARGET=LIQUID H{-2} 14B c Compiled (unevaluated) dataset from 2005Ka06: 14B 2c Phys Lett B 608, 206 (2005) 14B c Compiled by J. Roediger and B. Singh (McMaster) July 14, 2005 14B c Secondary beam of {+17}B produced by fragmentation of {+22}Ne primary 14B 2c beam on Be production target at E=110 MeV/nucleon. Incident beam 14B 3c identified using time-of-flight between scintillators placed at two 14B 4c achromatic foci of fragment separator, combined with magnetic rigidity 14B 5c and energy loss information. Particle identification done using |DE-E 14B 6c while a Si telescope was used to detect and identify {+17}B scattered 14B 7c projectile and reaction products after the H{-2} target. Energy of 14B 8c {+17}B at target mid-plane was |?43 MeV / nucleon. 14B c Measured E|g, I|g, fragment-|g coin with the DALI2 array of 158 NaI(Tl) 14B 2c crystals and a Si telescope. 14B cG E$Uncertainty of target thickness introduces error of |?5 keV in peak 14B 2cG position determination. Doppler correction done event by event and 14B 3cG confirmed by agreement in observed peak position of 953 transition from 14B 4cG {+12}B. 14B cG E$1089 keV transition from {+17}B is observed by 2005Ka06 in {+14}B 14B 2cG spectrum. The authors attribute this to tertiary reactions from 14B 3cG the reaction target or from non-target materials downstream of the 14B 4cG target and is not due to background from particle identification. 14B cL J$From {+14}B in ENSDF. 14B L 0.0 2- 14B L 654 9 (1-) 14B cL E$excited state in {+14}B possible result of only neutron excitation 14B 2cL (from systematics of neighboring boron isotopes). 14B G 654 9 14B cG E$possible new determination of 740 keV {I40} |g peak observed earlier 14B 2cG by 1973Ba34. 14B 1H(14BE,14B):XUNDL-2 2011SA02 201105 14B c Compiled (unevaluated) dataset from 2011Sa02 14B c Phys Lett B 697, 459 (2011) 14B c Compiled by J. Kelley and C.G. Sheu (TUNL), May 02, 2011. 14B c The authors measured the {+14}Be(p,n){+14}B charge-exchange reaction in 14B 2c inverse kinematics at E({+14}Be)=69 MeV/nucleon. A beam of 100 14B 3c MeV/nucleon {+18}O was fragmented on a thick {+9}Be target to produce 14B 4c a beam of 69 MeV/nucleon {+14}Be ions at the RIPS facility at RIKEN. 14B 5c The {+14}Be beam impinged on a 3 cm diameter by 229 (6) mg/cm{+2} 14B 6c liquid hydrogen target. The {+13}B+n events were detected and the 14B 7c {+14}B excitation spectrum was determined from kinematics. The {+13}B 14B 8c kinematics were measured by a set of position sensitive multi-wire 14B 9c drift chambers (positioned after a dipole) and plastic |DE-E 14B ac hodoscope; neutrons were detected via two plastic scintillator walls; 14B bc and no |g-rays were detected in coincidence with {+13}B+n pairs. A 14B cc DWBA analysis of the reconstructed angular distributions permitted an 14B dc analysis of the |b(GT) for the J|p=1+, E{-x} |?1.3 MeV state as well 14B ec as analysis of the J|p values of the observed states. 14B c Target J|p=1/2+. 14B CL T$LABEL=WIDTH 14B L 1.27E3 2 1+ 160 KEV 20 1 14B cL E$from E({+13}B+n)=304 keV {I4}. 14B L 2.08E3 4- 2 14B cL E$from (1973Ba34, 2000Ka21). 14B L 4.06E3 5 (3+,3-) 1.2 MEV 5 (1,2) 14B cL T$for L=2. |G=1.0 MeV {I3} for L=1 14B cL E$from E({+13}B+n)=3090 keV {I50}. 14B 2H(13B,P):XUNDL-3 2013BE25 201308 14B c Compiled (unevaluated) dataset from 2013Be25 14B c Phys Rev C 88, 011304(R) (2013) 14B c Compiled by J. Kelley and C.G. Sheu (TUNL), August 05, 2013. 14B c The authors measured the {+13}B(d,p){+14}B reaction in inverse 14B 2c kinematics, as a means to study the level properties of {+14}B. 14B c A beam of E({+13}B)=204 MeV ions (|DE |? 5 MeV), produced via the 14B 2c {+9}Be({+14}C,{+13}B) reaction at the ANL/ATLAS facility, impinged on 14B 3c a 220 |mg/cm{+2} Cd{-2} foil that was positioned at the target position 14B 4c for the HELIOS Si detector array. The {+14}|b{++}p reaction products 14B 5c were detected in coincidence to minimize events caused by beam 14B 6c impurities; protons emitted at |q > 90|' were detected in the HELIOS, 14B 7c while scattered {+13}B and {+14}B ions were detected in an array of 14B 8c four Si |DE-E telescopes that covered |q=0.5|' to 2.8|'. 14B c The excitation energy spectrum is deduced by evaluating p+{+14}B 14B 2c coincidence events for states below the neutron separation energy (S(n) 14B 3c |? 970 keV) and p+{+13}B events for states above the separation energy. 14B 4c Four peaks are observed in the spectrum, which are associated with the 14B 5c first J|p=2-, 1-, 3- and 4- states. 14B c The scattered proton angular distributions are analyzed via DWBA, and 14B 2c relative spectroscopic factors are deduced for the {Il}=0 and 2 14B 3c components. Two additional states at E{-x}=1.86 and 4.5 MeV with J|p=2- 14B 4c and 1-, respectively are unobserved, but are evaluated. 14B cL E$From Adopted Levels of {+14}B in ENSDF database, except where noted. 14B CL T$LABEL=WIDTH 14B cL S$ Relative to 1.0 for E{-x}=1.38 MeV 14B L 0 2- 0+2 14B cL $S({Il}=0)=0.71 {I5}(fit) {I14}(theory) and S({Il}=2)=0.17 {I5}(fit) 14B 2cL {I4}(theory). 14B L 654 9 1- 0(+2) 0.94 28 14B cL E$from 2005Ka06. 14B cL $S({Il}=0)=0.94 {I20}(fit) {I20}(theory) and S({Il}=2) |< 0.06. 14B L 1380 30 (3-) 2 1.00 14B cL $S({Il}=2) is defined as unity. 14B L 2080 50 (4-) 200 KEV 50 2 1.00 22 14B cL $S({Il}=2)=1.00 {I10}(fit) {I20}(theory). 14B 9BE(14B,X):RADIUS:XUNDL-4 2014ES07 201411 14B c Compiled (unevaluated) dataset from 2014Es07 14B c Phys Rev Lett 113, 132501 (2014) 14B c Compiled by J. Kelley and C.G. Sheu (TUNL), November 17, 2014. 14B c The authors measured the charge changing reaction cross sections of 14B 2c boron isotopes and deduced their root mean square proton radii. 14B c Beams of |? 850 - 900 MeV/nucleon boron isotopes were produced by 14B 2c fragmenting {+22}Ne({+10,14-17}B) and {+40}Ar({+11-13}B) ions on a 14B 3c thick {+9}Be foil at the GSI/FRS fragment separator. The beam species 14B 4c were identified by |DE (ionization chamber) vs time-of-flight before 14B 5c they impinged on a 4.010 g/cm{+2} thick carbon target. An ionization 14B 6c chamber located after the target was used to identify charge changing 14B 7c reaction events. 14B c In the discussion, the rms proton radii for {+10,11}B are obtained from 14B 2c e{+-} and |p{+-} scattering and muonic x-ray studies, while for heavier 14B 3c boron isotopes the proton radii are obtained by analyzing the charge 14B 4c changing cross sections, |s{-|a}, in a Glauber model. Finally, the rms 14B 5c proton radii are compared with rms matter radii derived from 14B 6c interaction cross section measurements in the literature. 14B cL E,J$From Adopted Levels of {+14}B in ENSDF database. 14B L 0 2- 14B cL ${Ir}{-rms}(proton)=2.50 fm {I2} obtained from Glauber model analysis 14B 2cL of the charge changing cross section |s{-|a}=727 mb {I4} at 14B 3cL E({+14}B)=926 MeV/nucleon 14B 15C(D,3HE):XUNDL-5 2016BE08 201609 14B c Compiled (unevaluated) dataset from 2016Be08 14B c Phys. Rev. C 93, 044323 (2016) 14B c Compiled by J.H. Kelley (TUNL), T. Truong (TUNL-REU) and C.G. Sheu 14B 2c (TUNL), June 30, 2016. 14B c The authors analyzed the angular distributions of {+3}He particles 14B 2c from the {+15}C(d,{+3}He){+14}B proton-removal reaction, in inverse 14B 3c kinematics, to study the J|p values of {+14}B states involved in the 14B 4c reaction. 14B c A beam of 15.7 MeV/nucleon {+15}C ions, produced in the 14B 2c d({+14}C,{+15}C)p reaction at the ANL/ATLAS facility, impinged on 140 14B 3c |mg/cm{+2}(Cd{-2}){-n} polyethylene foils located at the HELIcal 14B 4c Orbit Spectrometer (HELIOS) target position. The kinematics of {+3}He 14B 5c particles from (d,{+3}He) reactions were determined from analysis of 14B 6c the HELIOS array data, while recoiling boron isotopes were detected 14B 7c in set of silicon detector |DE-E telescopes that covered 14B 8c |q{-lab}=1|'-5|'. The resolution for excitation energies was found as 14B 9c |?240 keV FWHM. Angular distributions were analyzed via DWBA to 14B ac obtain L, J|p and C{+2}S values 14B c The {+3}He particle reaction data were analyzed in coincidence with 14B 2c any boron isotope to give access to population of unbound states. 14B CL T$LABEL=WIDTH 14B CL S$LABEL=C{+2}S 14B cL J$From the Adopted Levels of {+14}B in the ENSDF database, except 14B 2cL where noted. 14B L 0 2- 1 1.80 35 14B cL L$from sum of d|s/d|W for ground state and 650-keV level 14B L 0.65E3 1- 1 1.40 30 14B cL L$from sum of d|s/d|W for ground state and 650-keV level 14B L 1.8E3 3 (2-) 1 MEV AP 1 0.80 15 14B cL J$from measured L and comparison of C{+2}S with shell model 14B 2cL calculations