scholarly journals High-energy string scatterings of compactified open string

2008 ◽  
Vol 804 (1-2) ◽  
pp. 250-261 ◽  
Author(s):  
Jen-Chi Lee ◽  
Tomohisa Takimi ◽  
Yi Yang
Keyword(s):  
1989 ◽  
Vol 326 (1) ◽  
pp. 73-107 ◽  
Author(s):  
David J. Gross ◽  
J.L. Mañes

2013 ◽  
Vol 21 ◽  
pp. 153-154
Author(s):  
CHUAN-TSUNG CHAN ◽  
SHOICH KAWAMOTO ◽  
DAN TOMINO

It is known that infinitely many linear relations among string scattering amplitudes appear in high energy limit. These linear relations would imply a symmetry structure that is not manifest before taking the high energy limit. Motivated by this observation, we study an effective field theory of massive spin-2 and spin-1 particles, and try to understand what kind of structure reproduces the linear relations among the amplitudes of bosonic open string.


2006 ◽  
Vol 749 (1-3) ◽  
pp. 266-279 ◽  
Author(s):  
Chuan-Tsung Chan ◽  
Pei-Ming Ho ◽  
Jen-Chi Lee ◽  
Shunsuke Teraguchi ◽  
Yi Yang

2005 ◽  
Vol 725 (1-2) ◽  
pp. 352-382 ◽  
Author(s):  
Chuan-Tsung Chan ◽  
Pei-Ming Ho ◽  
Jen-Chi Lee ◽  
Shunsuke Teraguchi ◽  
Yi Yang

2020 ◽  
Vol 2020 (8) ◽  
Author(s):  
Cheuk-Yin Wong

AbstractAs a quark and an antiquark cannot be isolated, the intrinsic motion of a composite $$ q\overline{q} $$ q q ¯ system in its lowest-energy states lies predominantly in 1+1 dimensions, as in an open string with the quark and the antiquark at its two ends. Accordingly, we study the lowest-energy states of an open string $$ q\overline{q} $$ q q ¯ system in QCD and QED in 1+1 dimensions. We show that π0, η, and η′ can be adequately described as open string $$ q\overline{q} $$ q q ¯ QCD mesons. By extrapolating into the $$ q\overline{q} $$ q q ¯ QED sector in which a quark and an antiquark interact with the QED interaction, we find an open string isoscalar I(Jπ) = 0(0−) QED meson state at 17.9±1.5 MeV and an isovector (I(Jπ) = 1(0−), I3 = 0) QED meson state at 36.4±3.8 MeV. The predicted masses of the isoscalar and isovector QED mesons are close to the masses of the hypothetical X17 and E38 particles observed recently, making them good candidates for these particles. The decay products of QED mesons may show up as excess e+e− and γγ pairs in the anomalous soft photon phenomenon associated with hadron productions in high-energy hadron-proton collisions and e+-e− annihilations. Measurements of the invariant masses of excess e+e− and γγ pairs will provide tests for the existence of the open string $$ q\overline{q} $$ q q ¯ QED mesons. An assembly of gravitating QED mesons are expected to emit electron-positron pairs and/or gamma rays and their decay energies and lifetimes will be modified by their gravitational binding energies. Consequently, a self-gravitating isoscalar QED meson assembly whose mass M and radius R satisfy (M/M⨀)/(R/R⨀) ≳ 2 4.71 × 105 will not produce electron-positron pairs nor gamma rays and may be a good candidate for the primordial dark matter.


2012 ◽  
Vol 27 (13) ◽  
pp. 1250070 ◽  
Author(s):  
I. Y. PARK

In the full type IIB open superstring setup, we show that there exists a vertex operator, denoted by VL, whose renormalization reproduces the same anomalous dimension matrix that was obtained by Minahan and Zarembo (MZ) [J. High Energy Phys. 0303, 013 (2003)]. The vertex operator is a gauge singlet, and has the same SO(6) index structure as the operator used by MZ. To obtain the SYM anomalous dimensions, one of the key ingredients is the non-abelianization of the nonlinear sigma model action in a D-brane background. Park [Phys. Lett. B 660, 583 (2008)] conjectured that quantum effects of open strings on a stack of D-branes should generate the curvature. Even though the conjecture had passed a few consistency checks, the role of the higher order curvature terms has remain mostly unobserved until now. By choosing a special form of the non-abelianized counter vertex, VG, we show that the SYM result is reproduced. We comment on fermionic completion of VL and on how the special form of the non-Abelian vertex VG may arise.


2001 ◽  
Vol 499 (1-2) ◽  
pp. 158-166 ◽  
Author(s):  
Tsunehide Kuroki ◽  
Soo-Jong Rey

1984 ◽  
Vol 75 ◽  
pp. 599-602
Author(s):  
T.V. Johnson ◽  
G.E. Morfill ◽  
E. Grun

A number of lines of evidence suggest that the particles making up the E-ring are small, on the order of a few microns or less in size (Terrile and Tokunaga, 1980, BAAS; Pang et al., 1982 Saturn meeting; Tucson, AZ). This suggests that a variety of electromagnetic and plasma affects may be important in considering the history of such particles. We have shown (Morfill et al., 1982, J. Geophys. Res., in press) that plasma drags forces from the corotating plasma will rapidly evolve E-ring particle orbits to increasing distance from Saturn until a point is reached where radiation drag forces acting to decrease orbital radius balance this outward acceleration. This occurs at approximately Rhea's orbit, although the exact value is subject to many uncertainties. The time scale for plasma drag to move particles from Enceladus' orbit to the outer E-ring is ~104yr. A variety of effects also act to remove particles, primarily sputtering by both high energy charged particles (Cheng et al., 1982, J. Geophys. Res., in press) and corotating plasma (Morfill et al., 1982). The time scale for sputtering away one micron particles is also short, 102 - 10 yrs. Thus the detailed particle density profile in the E-ring is set by a competition between orbit evolution and particle removal. The high density region near Enceladus' orbit may result from the sputtering yeild of corotating ions being less than unity at this radius (e.g. Eviatar et al., 1982, Saturn meeting). In any case, an active source of E-ring material is required if the feature is not very ephemeral - Enceladus itself, with its geologically recent surface, appears still to be the best candidate for the ultimate source of E-ring material.


Author(s):  
J. B. Warren

Electron diffraction intensity profiles have been used extensively in studies of polycrystalline and amorphous thin films. In previous work, diffraction intensity profiles were quantitized either by mechanically scanning the photographic emulsion with a densitometer or by using deflection coils to scan the diffraction pattern over a stationary detector. Such methods tend to be slow, and the intensities must still be converted from analog to digital form for quantitative analysis. The Instrumentation Division at Brookhaven has designed and constructed a electron diffractometer, based on a silicon photodiode array, that overcomes these disadvantages. The instrument is compact (Fig. 1), can be used with any unmodified electron microscope, and acquires the data in a form immediately accessible by microcomputer.Major components include a RETICON 1024 element photodiode array for the de tector, an Analog Devices MAS-1202 analog digital converter and a Digital Equipment LSI 11/2 microcomputer. The photodiode array cannot detect high energy electrons without damage so an f/1.4 lens is used to focus the phosphor screen image of the diffraction pattern on to the photodiode array.


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