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J. Esparza

Florida State University · US
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Area of research
Nuclear and High Energy Physics · Radiation
Research interest
Research topics from publications: Ti50(d,p)Ti51: Single-neutron energies in the N; SABRE: The Silicon Array for Branching Ratio Experiments; Fe54(d,p)Fe55 and the evolution of single neutron energies in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"; The CeBrA demonstrator for particle-γ coincidence experiments at the FSU Super-Enge Split-Pole Spectrograph; g9/2 neutron strength in the N=29 isotones and the Cr<mml:non; Measurement of g9/2 strength in the stretched 8− state and other negative parity states via the <mml:mi mathvaria; Single-neutron adding on $$^{34}$$S. Representative work: A measurement of the $^{50}\mathrm{Ti}(d,p)^{51}\mathrm{Ti}$ reaction at 16 MeV was performed using the Super Enge Split-Pole Spectrograph to measure the magnitude of the $N=32$ subshell gap in Ti. Seven states were observed that had not been observed in previous $(d,p)$ measurements, and the $L$ transfer values for six previously measured states were either changed or measured for the first time. The results were used to determine single neutron energies for the ${p}_{3/2}$, ${p}_{1/2}$, and ${f}_{5/2}$ orbitals. The resulting single neutron energies in $^{51}\mathrm{Ti}$ confirm the existence of the $N=32$ gap in Ti. These single neutron energies and those from previous measurements in $^{ A measurement of the $^{54}\mathrm{Fe}(d,p)^{55}\mathrm{Fe}$ reaction at 16 MeV was performed using the Florida State University Super-Enge Split-Pole Spectrograph to determine single-neutron energies for the $2{p}_{3/2}, 2{p}_{1/2}, 1{f}_{5/2}, 1{g}_{9/2}$, and $2{d}_{5/2}$ orbits. Two states were observed that had not been observed in previous ($d,p$) measurements. In addition, we made angular momentum transfer, $L$, assignments to four states and changed $L$ assignments from previous ($d,p$) measurements for nine more states. The spin-orbit splitting between the $2{p}_{3/2}$ and $2{p}_{1/2}$ orbits is similar to that in the other $N=29$ isotones and not close to zero as a previous measure
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Recent publications

Measurement of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mn>9</mml:mn><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:math> strength in the stretched <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msup><mml:mn>8</mml:mn><mml:mo>−</mml:mo></mml:msup></mml:math> state and other negative parity states via the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi mathvaria
Physical review. C 2024cited by 3position: middledoi
Single-neutron adding on $$^{34}$$S
The European Physical Journal A 2024cited by 1position: middledoi
The CeBrA demonstrator for particle-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si90.svg" display="inline" id="d1e1256"><mml:mi>γ</mml:mi></mml:math> coincidence experiments at the FSU Super-Enge Split-Pole Spectrograph
Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment 2023cited by 7position: middledoi
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mn>9</mml:mn><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:math> neutron strength in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn>29</mml:mn></mml:mrow></mml:math> isotones and the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi>Cr</mml:mi><mml:mprescripts/><mml:non
Physical review. C 2023cited by 4position: middledoi
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi>Fe</mml:mi><mml:mprescripts/><mml:none/><mml:mn>54</mml:mn></mml:mmultiscripts><mml:mo>(</mml:mo><mml:mi>d</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mmultiscripts><mml:mi>Fe</mml:mi><mml:mprescripts/><mml:none/><mml:mn>55</mml:mn></mml:mmultiscripts></mml:mrow></mml:math> and the evolution of single neutron energies in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"
Physical review. C 2022cited by 8position: middledoi
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi>Ti</mml:mi><mml:mprescripts/><mml:none/><mml:mn>50</mml:mn></mml:mmultiscripts><mml:mo>(</mml:mo><mml:mi>d</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mmultiscripts><mml:mi>Ti</mml:mi><mml:mprescripts/><mml:none/><mml:mn>51</mml:mn></mml:mmultiscripts></mml:mrow></mml:math>: Single-neutron energies in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>N
Physical review. C 2021cited by 9position: middledoi
SABRE: The Silicon Array for Branching Ratio Experiments
Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment 2021cited by 8position: middledoi

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No grants ingested yet.

Frequent collaborators

I. Wiedenhöver · Florida State University5 papers (2021–2024)L. T. Baby · Indiana University Bloomington5 papers (2021–2024)G. W. McCann · Florida State University5 papers (2021–2024)K. Hanselman · Florida State University5 papers (2021–2024)K. W. Kemper · Florida State University4 papers (2021–2024) · 4 papers (2021–2024)P. D. Cottle · Florida State University4 papers (2021–2024)R. Renom · Florida State University3 papers (2022–2024)A. L. Conley · Florida State University3 papers (2022–2024)K. T. Macon · Florida State University3 papers (2021–2022)I. C. S. Hay · Florida State University3 papers (2022–2024)M. Spieker · Michigan State University3 papers (2022–2024)B. Kelly · Florida State University3 papers (2022–2024) · 2 papers (2023–2024) · 2 papers (2023–2024)E. Temanson · Oak Ridge National Laboratory2 papers (2021–2021)C. Benetti · Florida State University1 papers (2021–2021)E. Rubino · Michigan State University1 papers (2021–2021)Jesus Perello · Florida State University1 papers (2021–2021) · 1 papers (2022–2022)
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