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Journal Articles

Event structure and double helicity asymmetry in jet production from polarized $$p + p$$ collisions at $$sqrt{s}$$ = 200 GeV

Adare, A.*; Afanasiev, S.*; Aidala, C.*; Ajitanand, N. N.*; Akiba, Y.*; Al-Bataineh, H.*; Alexander, J.*; Aoki, K.*; Aphecetche, L.*; Armendariz, R.*; et al.

Physical Review D, 84(1), p.012006_1 - 012006_18, 2011/07

 Times Cited Count:29 Percentile:72.31(Astronomy & Astrophysics)

We report on the event structure and double helicity asymmetry ($$A_{LL}$$) of jet production in longitudinally polarized $$p + p$$ collisions at $$sqrt{s}$$ = 200 GeV. Photons and charged particles were measured by the PHENIX experiment. Event structure was compared with the results from PYTHIA event generator. The production rate of reconstructed jets is satisfactorily reproduced with the next-to-leading-order perturbative QCD calculation. We measured $$A_{LL}$$ = -0.0014 $$pm$$ 0.0037 at the lowest $$P_T$$ bin and -0.0181 $$pm$$ 0.0282 at the highest $$P_T$$ bin. The measured $$A_{LL}$$ is compared with the predictions that assume various $$Delta G(x)$$ distributions.

Journal Articles

Identified charged hadron production in $$p + p$$ collisions at $$sqrt{s}$$ = 200 and 62.4 GeV

Adare, A.*; Afanasiev, S.*; Aidala, C.*; Ajitanand, N. N.*; Akiba, Yasuyuki*; Al-Bataineh, H.*; Alexander, J.*; Aoki, Kazuya*; Aphecetche, L.*; Armendariz, R.*; et al.

Physical Review C, 83(6), p.064903_1 - 064903_29, 2011/06

 Times Cited Count:184 Percentile:99.44(Physics, Nuclear)

Transverse momentum distributions and yields for $$pi^{pm}, K^{pm}, p$$, and $$bar{p}$$ in $$p + p$$ collisions at $$sqrt{s}$$ = 200 and 62.4 GeV at midrapidity are measured by the PHENIX experiment at the RHIC. We present the inverse slope parameter, mean transverse momentum, and yield per unit rapidity at each energy, and compare them to other measurements at different $$sqrt{s}$$ collisions. We also present the scaling properties such as $$m_T$$ and $$x_T$$ scaling and discuss the mechanism of the particle production in $$p + p$$ collisions. The measured spectra are compared to next-to-leading order perturbative QCD calculations.

Journal Articles

Azimuthal correlations of electrons from heavy-flavor decay with hadrons in $$p+p$$ and Au+Au collisions at $$sqrt{s_{NN}}$$ = 200 GeV

Adare, A.*; Afanasiev, S.*; Aidala, C.*; Ajitanand, N. N.*; Akiba, Yasuyuki*; Al-Bataineh, H.*; Alexander, J.*; Aoki, Kazuya*; Aphecetche, L.*; Aramaki, Y.*; et al.

Physical Review C, 83(4), p.044912_1 - 044912_16, 2011/04

 Times Cited Count:9 Percentile:49.7(Physics, Nuclear)

Measurements of electrons from the decay of open-heavy-flavor mesons have shown that the yields are suppressed in Au+Au collisions compared to expectations from binary-scaled $$p+p$$ collisions. Here we extend these studies to two particle correlations where one particle is an electron from the decay of a heavy flavor meson and the other is a charged hadron from either the decay of the heavy meson or from jet fragmentation. These measurements provide more detailed information about the interaction between heavy quarks and the quark-gluon matter. We find the away-side-jet shape and yield to be modified in Au+Au collisions compared to $$p+p$$ collisions.

Journal Articles

Measurement of neutral mesons in $$p$$ + $$p$$ collisions at $$sqrt{s}$$ = 200 GeV and scaling properties of hadron production

Adare, A.*; Afanasiev, S.*; Aidala, C.*; Ajitanand, N. N.*; Akiba, Y.*; Al-Bataineh, H.*; Alexander, J.*; Aoki, K.*; Aphecetche, L.*; Armendariz, R.*; et al.

Physical Review D, 83(5), p.052004_1 - 052004_26, 2011/03

 Times Cited Count:177 Percentile:98.48(Astronomy & Astrophysics)

The PHENIX experiment at RHIC has measured the invariant differential cross section for production of $$K^0_s$$, $$omega$$, $$eta'$$ and $$phi$$ mesons in $$p + p$$ collisions at $$sqrt{s}$$ = 200 GeV. The spectral shapes of all hadron transverse momentum distributions are well described by a Tsallis distribution functional form with only two parameters, $$n$$ and $$T$$, determining the high $$p_T$$ and characterizing the low $$p_T$$ regions for the spectra, respectively. The integrated invariant cross sections calculated from the fitted distributions are found to be consistent with existing measurements and with statistical model predictions.

JAEA Reports

Field testing of near-real-time materials accountancy at the PNC-TOKAI reprocessing plant

; ; Iwanaga, Masayuki; Todokoro, Akio; ; Masui, Jinichi; Miura, Nobuyuki*; Lovett, J. E.*

PNC TN8410 86-52, 66 Pages, 1987/01

PNC-TN8410-86-52.pdf:1.61MB

None

JAEA Reports

In-plant Measurements of Gamma-ray Transmissions for Precise K-edge and Passive Assay of Plutonium Concentration and Isotopic Fractions in Product Solutions

Russo, P. A.*; Asakura, Yoshiro*; Hsue, S. T.*; Kondo, Isao*; Sprinkle, J. K. Jr.*; Masui, J.*; Johnson, S. S.*; Shoji, J.*

PNC TN841 82-10, 76 Pages, 1982/08

PNC-TN841-82-10.pdf:4.87MB

An instrument based upon high-resolution $$gamma$$-ray measurements has beentested for more than 1 year at the TokaiReprocessing Facility for determinationof plutonium concentration by K-edge absorption densitometry and for determination of plutonium isotopic fractions bytransmission-corrected passive $$gamma$$-ray spectrometry. The nondestructive assay instrument was designed and built atLos Alamos National Laboratory for theTokai Advanced Safeguards Technology Exercise (TASTEX). It was used at Tokai forthe timely assay of more than 100 productsolution samples daring the TASTEX evaluations The results were compared tosolution samples during the TASTEXaluations. The results were compared toreference values obtained by conventionaldestructive analysis of these samples. The precision and accuracy of plutoniumconcentrations measured by the K-edgetechnique are shown to be with in 0.6% (1$$sigma$$) in these applications. The precisionsand accuracies of the isotopic fractions. determined by these passive

JAEA Reports

None

Asakura, Yoshiro*; Miyahara, Kenji; *; Masui, J.*; Kondo, Isao*; *; *; Kamata, Masayuki

PNC TN852 81-18, 266 Pages, 1981/05

PNC-TN852-81-18.pdf:6.24MB

None

JAEA Reports

None

Miyahara, Kenji; Asakura, Yoshiro*; *; Masui, J.*; Kondo, Isao*; *; Kamata, Masayuki; *

PNC TN852 81-15, 46 Pages, 1981/04

PNC-TN852-81-15.pdf:2.23MB

None

JAEA Reports

None

*; Masui, J.*; Tsuboya, Takao*

PNC TN841 77-59, 34 Pages, 1977/11

PNC-TN841-77-59.pdf:0.97MB

no abstracts in English

JAEA Reports

None

Tsuboya, Takao*; Kamata, Masayuki; Wada, Yukio; Masui, J.*; *; Wada, Tsutomu*; ; *

PNC TN851 76-01, 42 Pages, 1976/01

PNC-TN851-76-01.pdf:1.26MB

None

Oral presentation

Ultra-small-angle neutron scattering study of Actin-Polymer complexes formation

Masui, Tomomi; Koizumi, Satoshi; Hashimoto, Takeji; Iwase, Hiroki; Shikinaka, Kazuhiro*; Kwon, H.*; Kakugo, Akira*; Gong, J.*

no journal, , 

no abstracts in English

Oral presentation

The Structure formation of filamentous actin and polycation complex

Masui, Tomomi; Shikinaka, Kazuhiro*; Kwon, H.*; Koizumi, Satoshi; Hashimoto, Takeji; Iwase, Hiroki; Kakugo, Akira*; Gong, J.*

no journal, , 

no abstracts in English

Oral presentation

Ultra-small angle neutron scattering observation of filamentous actin and polycation complex

Masui, Tomomi; Shikinaka, Kazuhiro*; Kwon, H.*; Koizumi, Satoshi; Hashimoto, Takeji; Iwase, Hiroki; Kakugo, Akira*; Gong, J.*

no journal, , 

no abstracts in English

Oral presentation

In situ observation on hierarchical actin bundle network

Masui, Tomomi; Shikinaka, Kazuhiro*; Kwon, H.*; Koizumi, Satoshi; Hashimoto, Takeji; Iwase, Hiroki; Kakugo, Akira*; Gong, J.*

no journal, , 

Actin is one of the most abundant cytoskeleton proteins in eucaryotic cell. They play a crucialrole in cell motility by polymerizing monomeric globular G-actin into polymeric filamentous actin (F-actin). With actin-binding proteins (ABPs), they form higher order structures such as linear bundles, two-dimensional networks and three-dimensional gels. It has been considered that these structures are controlled by ABPs. However recent study have shown that the only one kind of artificial cationic polymer can form variety of structures depending its concentration and salt concentration. This system is a good model to elucidate the mechanism of regulation of actin and ABPs complex structure. Based on these backgrounds, we have investigated the effects of salt concentration on the stability and structure of actin-polycation complexes by using small angle neutron scattering (SANS) technique.

Oral presentation

The Observation of structure formation of F-actin

Masui, Tomomi; Shikinaka, Kazuhiro*; Kwon, H.*; Koizumi, Satoshi; Hashimoto, Takeji; Iwase, Hiroki; Kakugo, Akira*; Gong, J.*

no journal, , 

no abstracts in English

Oral presentation

In situ observation on hierarchical actin bundle networks; Salt concentration effects

Masui, Tomomi; Shikinaka, Kazuhiro*; Kwon, H.*; Koizumi, Satoshi; Hashimoto, Takeji; Iwase, Hiroki; Kakugo, Akira*; Gong, J.*

no journal, , 

Actin is one of the cytoskeleton proteins and it is most abundant proteins in eucaryotic cell. They play a crucial role in cell motility by polymerization of monomeric globular G-actin into polymeric filamentous actin (F-actin). With actin binding proteins, they form various structures such as linear bundles, two-dimensional networks, and three-dimensional gels. It has been considered that these structures are controlled by the specific interaction between actin and binding protein. However from the physicochemical point of view, actin has negative charge and actin-binding protein has positive charge. Thus, the electrostatic interaction might play important role to determinein the structure. Based on this idea, we have investigated the effects of salt concentration on the stability and structure of actin-polymer complexes by using small angle neutron scattering (SANS) technique.

Oral presentation

Assembly and disassembly of actin and cationic polymer complex

Masui, Tomomi; Shikinaka, Kazuhiro*; Kwon, H.*; Koizumi, Satoshi; Hashimoto, Takeji; Iwase, Hiroki; Kakugo, Akira*; Gong, J.*

no journal, , 

Actin is one of the cytoskeleton proteins and it is most abundant proteins in eucaryotic cell. They play a crucial role in cell motility by polymerization of monomeric globular G-actin into polymeric filamentous actin (F-actin). With actin binding proteins, they form various structures such as linear bundles, two-dimensional networks, and three-dimensional gels. It has been considered that these structures are controlled by the specific interaction between actin and binding protein. However from the physicochemical point of view, actin has negative charge and actin-binding protein has positive charge. Thus, the electrostatic interaction might play important role to determine in the structure. Based on this idea, we have investigated the effects of salt concentration on the stability and structure of actin-polymer complexes by using small angle neutron scattering (SANS) technique.

Oral presentation

Assembly and disassembly of model cytoskeleton system

Masui, Tomomi; Shikinaka, Kazuhiro*; Kwon, H.*; Koizumi, Satoshi; Hashimoto, Takeji; Iwase, Hiroki; Kakugo, Akira*; Gong, J.*

no journal, , 

Actin is one of the most abundant cytoskeleton proteins in eucaryotic cell. They play a crucial role in cell motility by polymerizing monomeric globular G-actin into polymeric filamentous actin (F-actin). Withactin-binding proteins (ABPs), they form higher order structures such as linear bundles, two-dimensional networks and three-dimensional gels. In this study we have constructed model cytoskeleton system composed of F-actin, cationic polymer and salt. To investigate salt induced hierarchical structure change we employed fluorescence microscopy and small angle neutron scattering (SANS) technique.

Oral presentation

The Effect of salt on the hierarchical structure of F-actin/polycation complexes; In situ observation by fluorescnece microscopy and small angle neutron scattering

Masui, Tomomi; Shikinaka, Kazuhiro*; Koizumi, Satoshi; Hashimoto, Takeji; Kakugo, Akira*; Gong, J.*; Kwon, H.*

no journal, , 

We reconstituted in vitro model cytoskeleton using F-actin and polycation. We have investigated hierarchical structural change of F-actin/polycation complexes induced by salt quantitatively by fluorescence microscopy and small angle neutron scattering. Based on the obtained structural parameters, we will discuss dominant interactions which determine the structure.

Oral presentation

Salt induced hierarchical morphology change of actin/polycation complexes

Masui, Tomomi; Shikinaka, Kazuhiro*; Koizumi, Satoshi; Kakugo, Akira*; Hashimoto, Takeji; Gong, J.*

no journal, , 

Hierarchical structures of F-actin, an anionic polyelectrolyte, and PDMAPAA-Q, a synthetic linear cationic polyelectrolyte (polycation), complexes in KCl salt solutions have been examined over a wide range of length scales from nanometer to micrometer using a combination of ultra-small-angle neutron scattering technique and fluorescence microscopy. We found hierarchical condensation of actin/polycation complex composed of a superbundle of 10 micrometer, protobundle of 100 nanometer, and protofilament (F-actin) of nanometer. These structures are largely influenced by salt concentrations. With increase of salt concentration superbundle structure changes from globular to extended states, simultaneously, the regularity of F-actin inside the protobundle increased and protobundle size increased about ten times larger. Further increase of salt concentration brings the protobundle disassemble to single F-actin.

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