共查询到20条相似文献,搜索用时 31 毫秒
1.
In this article, we study the Λ
c
and Λ
b
baryons in the nuclear matter using the QCD sum rules, and obtain the in-medium masses
M\varLambda c*=2.335 GeVM_{\varLambda _{c}}^{*}=2.335~\mathrm{GeV},
M\varLambda b*=5.678 GeVM_{\varLambda _{b}}^{*}=5.678~\mathrm{GeV}, the in-medium vector self-energies
\varSigma \varLambda cv=34 MeV\varSigma ^{\varLambda _{c}}_{v}=34~\mathrm{MeV},
\varSigma \varLambda bv=32 MeV\varSigma ^{\varLambda _{b}}_{v}=32~\mathrm {MeV}, and the in-medium pole residues
l\varLambda c*=0.021 GeV3\lambda_{\varLambda _{c}}^{*}=0.021~\mathrm{GeV}^{3},
l\varLambda b*=0.026 GeV3\lambda_{\varLambda _{b}}^{*}=0.026~\mathrm{GeV}^{3}. The mass-shifts are
M\varLambda c*-M\varLambda c=51 MeVM_{\varLambda _{c}}^{*}-M_{\varLambda _{c}}=51~\mathrm{MeV} and
M\varLambda b*-M\varLambda b=60 MeVM_{\varLambda _{b}}^{*}-M_{\varLambda _{b}}=60~\mathrm{MeV}, respectively. 相似文献
2.
Haishan Liu Hui Luo Mingxing Luo Liucheng Wang 《The European Physical Journal C - Particles and Fields》2011,71(11):1793
This paper starts with a self-contained discussion of the so-called Akulov–Volkov action SAV\mathcal{S}_{\mathrm{AV}}, which is traditionally taken to be the leading-order action of the Goldstino field. Explicit expressions for SAV\mathcal{S}_{\mathrm{AV}} and its chiral version SAVch\mathcal{S}_{\mathrm{AV}}^{\mathrm{ch}} are presented. We then turn to the issue on how these actions are related to the leading-order action SNL\mathcal{S}_{\mathrm{NL}} proposed in the newly proposed constrained superfield formalism. We show that SNL\mathcal{S}_{\mathrm{NL}} may yield SAV/SAVch\mathcal{S}_{\mathrm {AV}}/\mathcal{S}_{\mathrm{AV}}^{\mathrm{ch}} or a totally different action SKS\mathcal{S}_{\mathrm{KS}}, depending on how the auxiliary field in the former is integrated out. However, SKS\mathcal{S}_{\mathrm{KS}} and SAV/SAVch\mathcal{S}_{\mathrm {AV}}/\mathcal{S}_{\mathrm{AV}}^{\mathrm{ch}} always yield the same S-matrix elements, as one would have expected from general considerations in quantum field theory. 相似文献
3.
4.
Li Lu Takashi Nishida Masahiro Echizen Yasuaki Ishikawa Kiyoshi Uchiyama Yukiharu Uraoka 《Applied Physics A: Materials Science & Processing》2013,112(2):425-430
Sol–gel-derived SrTa2O6 thin films were fabricated at a low temperature of 500 °C. To improve their leakage current properties, additional UV/O3-assisted annealing was performed from room temperature to 290 °C. UV/O3 treatment at 290 °C gave a very low leakage current that was six orders of magnitude lower than that of an untreated thin film. During UV/O3-assisted annealing, Si and Ti ions diffused from the substrates into the SrTa2O6 thin films and occupied the Ta5+ sites, subsequently generating Si? and Ti?. At a heating temperature of 290 °C, large amounts of Ti ions diffused throughout the SrTa2O6 thin film. These Ti ions contributed to the generation of inactive combinations of $(\mathrm{Si}^{-}\mbox{--}\mathrm{V}_{\mathrm{o}}^{+})^{+}\mbox{--}\mathrm{Ti}^{-}$ and $(\mathrm{Ti}^{-}\mbox{--}\mathrm{V}_{\mathrm{o}}^{+})^{+}\mbox{--}\mathrm{Ti}^{-}$ , which greatly reduced oxygen vacancies (Vo). Thus, the leakage current was significantly reduced. 相似文献
5.
Magnetocaloric properties of as-quenched Ni50.4Mn34.9In14.7 ferromagnetic shape memory alloy ribbons
Sánchez Llamazares J. L. García C. Hernando B. Prida V. M. Baldomir D. Serantes D. González J. 《Applied Physics A: Materials Science & Processing》2011,103(4):1125-1130
The temperature dependences of magnetic entropy change and refrigerant capacity have been calculated for a maximum field change
of Δ
H=30 kOe in as-quenched ribbons of the ferromagnetic shape memory alloy Ni50.4Mn34.9In14.7 around the structural reverse martensitic transformation and magnetic transition of austenite. The ribbons crystallize into
a single-phase austenite with the L21-type crystal structure and Curie point of 284 K. At 262 K austenite starts its transformation into a 10-layered structurally
modulated monoclinic martensite. The first- and second-order character of the structural and magnetic transitions was confirmed
by the Arrott plot method. Despite the superior absolute value of the maximum magnetic entropy change obtained in the temperature
interval where the reverse martensitic transformation occurs
(|\varDelta SMmax|=7.2 J kg-1 K-1)(|\varDelta S_{\mathrm{M}}^{\max}|=7.2\mbox{ J}\,\mbox{kg}^{-1}\,\mbox{K}^{-1}) with respect to that obtained around the ferromagnetic transition of austenite
(|\varDelta SMmax|=2.6 J kg-1 K-1)(|\varDelta S_{\mathrm{M}}^{\max}|=2.6\mbox{ J}\,\mbox{kg}^{-1}\,\mbox{K}^{-1}), the large average hysteretic losses due to the effect of the magnetic field on the phase transformation as well as the narrow
thermal dependence of the magnetic entropy change make the temperature interval around the ferromagnetic transition of austenite
of a higher effective refrigerant capacity (RCmagneff=95J kg-1\mathrm{RC}^{\mathrm{magn}}_{\mathrm{eff}}=95\mbox{J}\,\mbox{kg}^{-1} versus RCstructeff=60J kg-1)\mathrm{RC}^{\mathrm{struct}}_{\mathrm{eff}}=60\mbox{J}\,\mbox{kg}^{-1}). 相似文献
6.
Siegfried Bethke 《The European Physical Journal C - Particles and Fields》2009,64(4):689-703
Measurements of α
s, the coupling strength of the Strong Interaction between quarks and gluons, are summarised and an updated value of the world
average of as(MZ0)\alpha_{\mathrm{s}}(M_{\mathrm{Z}^{0}}) is derived. Special emphasis is laid on the most recent determinations of α
s. These are obtained from τ-decays, from global fits of electroweak precision data and from measurements of the proton structure function F2, which are based on perturbative QCD calculations up to O(as4)\mathcal{O}(\alpha_{\mathrm{s}}^{4}); from hadronic event shapes and jet production in e+e− annihilation, based on O(as3)\mathcal{O}(\alpha_{\mathrm{s}}^{3}) QCD; from jet production in deep inelastic scattering and from ϒ decays, based on O(as2)\mathcal{O}(\alpha_{\mathrm{s}}^{2}) QCD; and from heavy quarkonia based on unquenched QCD lattice calculations. A pragmatic method is chosen to obtain the world
average and an estimate of its overall uncertainty, resulting in
as(MZ0)=0.1184±0.0007.\alpha_\mathrm{s}(M_{\mathrm{Z}^0})=0.1184\pm 0.0007. 相似文献
7.
D. Atwood S. Bar-Shalom A. Soni 《The European Physical Journal C - Particles and Fields》2006,45(1):219-225
We describe a model for the scalar sector where all interactions occur either at an ultra-high scale, ΛU~1016-1019 GeV, or at an intermediate scale, ΛI = 109-1011 GeV. The interaction of physics on these two scales results in an SU(2) Higgs condensate at the electroweak (EW) scale, ΛEW, through a seesaw-like Higgs mechanism,
, while the breaking of the SM SU(2) x U(1) gauge symmetry occurs at the intermediate scale ΛI . The EW scale is, therefore, not fundamental but is naturally generated in terms of ultra-high energy phenomena and so the
hierarchy problem is alleviated. We show that the class of such "seesaw Higgs" models predict the existence of sub-eV neutrino
masses which are generated through a "two-step" seesaw mechanism in terms of the same two ultra-high scales:
. The neutrinos can be either Dirac or Majorana, depending on the structure of the scalar potential. We also show that our
seesaw Higgs model can be naturally embedded in theories with tiny extra dimensions of size
fm, where the seesaw induced EW scale arises from a violation of a symmetry at a distant brane; in particular, in the scenario
presented there are seven tiny extra dimensions.
Received: 19 August 2004, Revised: 27 July 2005, Published online: 14 October 2005 相似文献
8.
Time evolution of the Infrared Laser Induced Breakdown Spectroscopy of DNA bases Guanine and Adenine
L. Diaz L. Rubio J. J. Camacho 《Applied Physics A: Materials Science & Processing》2013,110(4):847-851
Laser-Induced Breakdown Spectroscopy (LIBS) of DNA bases Guanine and Adenine was studied using a high-power CO2 pulsed laser (λ=10.591 μm, τ FWHM=64 ns and fluences ranging from 25 to 70 J/cm2). The strong emission of the adenine and guanine plasma, collected using a high-resolution spectrometer, at medium-vacuum conditions (4 Pa) and at 1 mm from the target, exhibits excited molecular bands of CN (B2 Σ +–X2 Σ +) and excited neutral H and ionized N+ and C+. The medium-weak emission is due to excited species C2+, C3+, N, O, O+, O2+ and molecular band systems of $\mathrm{C}_{2}(\mathrm{d}^{3}\varPi_{\mathrm{g}}\mbox{--}\mathrm{a}^{3}\varPi_{\mathrm{u}};\ \mathrm{D}^{1}\varSigma_{\mathrm{u}}^{+}\mbox{--}\mathrm{X}^{1}\varSigma_{\mathrm{g}}^{+})$ , OH(A2 Σ +–X2 Π), NH(A3 Π–X3 Σ ?), CH(A2 Π–X2 Π), $\mathrm{N}_{2}^{+}(\mathrm{B}^{2}\varSigma_{\mathrm{u}}^{+}\mbox{--} \mathrm{X}^{2}\varSigma_{\mathrm{g}}^{+})$ and N2(C3 Π u–B3 Π g). We focus our attention on the temporal evolution of different atomic/ionic and molecular species. The velocity distributions for various (different) species were obtained from time-of-flight (TOF) measurements. Intensities of some lines from C+ were used for determining electron temperature and their Stark-broadened profiles were employed to estimate the temporal evolution of electron density. 相似文献
9.
S. Corradetti L. Biasetto M. Manzolaro D. Scarpa A. Andrighetto S. Carturan G. Prete P. Zanonato D. W. Stracener 《The European Physical Journal A - Hadrons and Nuclei》2011,47(10):119
The temperature dependence of neutron-rich isotope yields was studied within the framework of the HRIBF-SPES Radioactive Ion
Beams (RIB) project. On-line release measurements of fission fragments from a uranium carbide target at $\ensuremath 1600 {}^{\circ}\mathrm{C}$\ensuremath 1600 {}^{\circ}\mathrm{C} , 1800 °C\ensuremath 1800 {}^{\circ}\mathrm{C} and 2000 °C\ensuremath 2000 {}^{\circ}\mathrm{C} were performed at ORNL (USA). The fission reactions were induced by a 40MeV proton beam accelerated into a uranium carbide
target coupled to a plasma ion source. The experiments allowed for tests of performance of the SPES multi-foil target prototype
loaded with seven UC2/graphite discs (ratio C/U = 4 with density about 4g/cm3. 相似文献
10.
R. Enberg B. Pire L. Szymanowski S. Wallon 《The European Physical Journal C - Particles and Fields》2006,45(3):759-769
We calculate the leading order BFKL amplitude for the exclusive diffractive process
in the forward direction, which can be studied in future high energy e
+
e
- linear colliders. The resummation effects are very large compared to the fixed-order calculation. We also estimate the next-to-leading
logarithmic corrections to the amplitude by using a specific resummation of higher order effects and find a substantial growth
with energy, but smaller than in the leading logarithmic approximation.
CPHT Unité mixte 8627 du CNRS
LPT Unité mixte 8627 du CNRS
An erratum to this article is available at . 相似文献
11.
Massimo Franceschetti Mathew D. Penrose Tom Rosoman 《Journal of statistical physics》2011,142(3):460-486
We consider the supercritical finite-range random connection model where the points x,y of a homogeneous planar Poisson process are connected with probability f(|y−x|) for a given f. Performing percolation on the resulting graph, we show that the critical probabilities for site and bond percolation satisfy
the strict inequality $p_{c}^{\mathrm{site}} > p_{c}^{\mathrm{bond}}$p_{c}^{\mathrm{site}} > p_{c}^{\mathrm{bond}}. We also show that reducing the connection function f strictly increases the critical Poisson intensity. 相似文献
12.
E. A. Kataeva A. D. Bozhko S. V. Demishev 《Bulletin of the Lebedev Physics Institute》2010,37(11):347-351
The conductivity of carbon films grown by polymethylphenylsiloxane vapor decomposition in stimulated dc discharge plasma was
studied. It is found that the Mott hopping conductivity $
\sigma \left( T \right) = \sigma _0 \left( T \right)\exp \left\{ { - \frac{{T_0 }}
{T}^{{1 \mathord{\left/
{\vphantom {1 4}} \right.
\kern-\nulldelimiterspace} 4}} } \right\}
$
\sigma \left( T \right) = \sigma _0 \left( T \right)\exp \left\{ { - \frac{{T_0 }}
{T}^{{1 \mathord{\left/
{\vphantom {1 4}} \right.
\kern-\nulldelimiterspace} 4}} } \right\}
is characteristic of the samples under study in the temperature range of 80–400 K in the electric field E to 5 · 104 V/cm. An analysis of the pre-exponential factor σ
0(T) = σ
00(T
0)T
α allowed the conclusion that the hopping transport is most adequately described in the model with the exponential energy dependence
of the density of localized states for which α = −1/2 and the universal relation ln σ
00 −T
01/4 0 is valid, which is satisfied in the range where the parameter σ
00 varies by eight orders of magnitude. 相似文献
13.
Gruskova A. Lipka J. Papanova M. Kevicka D. Gonzalez A. Mendoza G. Toth I. Slama J. 《Hyperfine Interactions》2004,159(1-4):187-191
The β-NMR of short-lived β-emitter in a rutile TiO2 single crystal has been measured as functions of temperature and external magnetic field. Atomic motion induced spin lattice
relaxation was observed for two known sites, O substitutional and interstitial sites. The data were analyzed in terms of the
thermal atomic jump, which suggests that the motion of defects around the substitutional 12N atom for O, and of the interstitial 12N atom are attributed to the spin lattice relaxation. The electric field gradients have shown temperature dependence for both
sites, which is probably due to the thermal expansion of rutile. 相似文献
14.
The decay chain
is identified in a sample of 3.9 million hadronic Z decays collected with the OPAL detector at LEP. The branching ratio BR
is measured to be
for the J
P
=1+ (D0
1) state. For decays into the J
P
=2+ (D2
*0) state, an upper limit of 1.4 x 10-3 is placed on the branching ratio at the 95% confidence level.Received: 20 December 2002, Revised: 15 April 2003, Published online: 12 September 2003 相似文献
15.
V. ?vor?ík O. Kvítek O. Lyutakov J. Siegel Z. Kolská 《Applied Physics A: Materials Science & Processing》2011,102(3):747-751
Abstract The effects of annealing on gold structures sputtered onto glass substrate were studied using AFM, UV-Vis methods
and electrical measurements. The colour of the as-deposited films changes from blue to green with increasing deposition time.
After 1 hour annealing at 300°C the structures acquire red colour regardless of the film thickness. The annealing results
in dramatic changes of surface morphology and roughness and creation of relatively large “spherolytic and hummock-like” structures
in the gold layer. For deposited structures a non-zero optical band gap EgoptE_{\mathrm{g}}^{\mathrm{opt}} was determined from UV-Vis spectra using Tauc’s model and it indicates a semi-conducting character of the structures. The
annealing leads to an increase of the band gap. Electrical resistance of the deposited unannealed structures decreases dramatically
for deposition times above 50 s. For annealed structures the resistance fall comes until after 250 s deposition time. 相似文献
16.
T. Pandiyarajan R. Udayabhaskar B. Karthikeyan 《Applied Physics A: Materials Science & Processing》2012,107(2):411-419
In this report, Raman and Fourier Transform Infrared (FTIR) measurements were carried out to study the phonon modes of pure
and Fe doped ZnO nanoparticles. The nanoparticles were prepared by sol–gel technique at room temperature. The X-ray diffraction
measurements reveal that the nanoparticles are in hexagonal wurtzite structure and doping makes the shrinkage of the lattice
parameters, whereas there is no alteration in the unit cell. Raman measurements show both E2lowE_{2}^{\mathrm{low}} and E2HighE_{2}^{\mathrm{High}} optical phonon mode is shifted towards lower wave number with Fe incorporation and explained on the basis of force constant
variation, stress measurements, respectively. In addition, Fe related local vibrational modes (LVM) were observed for higher
concentration of Fe doping. FTIR spectra reveal a band at 444 cm−1 which is specific to E
1 (TO) mode; a red-shift of this mode in Fe doped samples and some surface phonon modes were observed. Furthermore, the observation
of additional IR modes, which is considered to have an origin related to Fe dopant in the ZnO nanostructures, is also reported.
These additional mode features can be regarded as an indicator for the incorporation of Fe ions into the lattice position
of the ZnO nanostructures. 相似文献
17.
In the structure-dynamic approach of nanoionics, the method of a uniform effective field \( {F}_{\mathrm{eff}}^{j,k} \) of a crystallographic planeX j has been substantiated for solid electrolyte nanostructures. The \( {F}_{\mathrm{eff}}^{j,k} \)is defined as an approximation of a non-uniform field \( {F}_{\mathrm{dis}}^j \)of X j with a discrete- random distribution of excess point charges. The parameters of \( {F}_{\mathrm{eff}}^{j,k} \)are calculated by correction of the uniform Gauss field \( {F}_{\mathrm{G}}^j \) of X j . The change in an average frequency of ionic jumps X k ?→?X k?+?1 between adjacent planes of nanostructure is determined by the sum of field additives to the barrier heights η k , k?+?1, and for \( {F}_{\mathrm{G}}^j \) and \( {F}_{\mathrm{dis}}^j \), these sums are the same decimal order of magnitude. For nanostructures with length ~4 nm, the application of \( {F}_{\mathrm{G}}^j \) (as \( {F}_{\mathrm{eff}}^{j,k} \)) gives the accuracy ~20 % in calculations of ion transport characteristics. The computer explorations of the “universal” dynamic response (Reσ ??∝?ω n ) show an approximately the same power n < ≈1 for\( {F}_{\mathrm{G}}^j \) and \( {F}_{\mathrm{eff}}^{j,k} \). 相似文献
18.
C. Karras C. M��hlig W. Paa T. Zeuner W. Triebel H. Stafast 《Applied physics. B, Lasers and optics》2011,104(1):17-20
Femtosecond (fs) laser pulses at variable delay times allowed us to track the fast non-radiative transitions between the manifold of highly excited $\mathrm{M}_{\mathrm{Na}}^{**}$ states to the lower lying fluorescent $\mathrm{M}_{\mathrm{Na}}^{*}$ state in CaF2. Two distinct $\mathrm{M}_{\mathrm{Na}}^{**}$ states of the manifold at 3.16?eV ( $\mathrm{M}_{\mathrm{Na}2}^{**}$ ) and 4.73?eV ( $\mathrm{M}_{\mathrm{Na}3}^{**}$ ) were populated using the second (SH) and third harmonics (TH) of fs laser light at 785?nm. The population kinetics of the fluorescent $\mathrm{M}_{\mathrm{Na}}^{*}$ state in the 2?eV excitation energy range was revealed by depleting its fluorescence centered at 740?nm using fundamental near infrared (NIR) fs laser pulses. The related time constants for $\mathrm{M}_{\mathrm{Na}2,3}^{**}{\sim}{>} \mathrm{M}_{\mathrm{Na}}^{*}$ relaxation amounted to 1.0±0.14?ps and 3.0±0.3?ps upon SH and TH excitation, respectively. 相似文献
19.
Y. Yoshida Y. Ino K. Matsumuro T. Watanabe H. Fujita K. Hayakawa K. Yukihira K. Ogai K. Moriguchi Y. Harada H. Soejima 《Hyperfine Interactions》2016,237(1):130
A prototype Mössbauer Spectroscopic Microscope is applied for the feasibility study of 57Fe impurity diffusion in Si wafers. A 2nm- 57Fe deposited Si wafer is annealed at 430 °C for 1 hour, and subsequently the 1/3 area of the wafer is further grinded with an angle of 6 degrees to the original surface to get a higher depth resolution for the mapping. Subsequently, the mapping images for Fe\(_{\text {sub}}^{\mathrm {0}}\), Fe\(_{\text {int}}^{\mathrm {0}}\), and Fe\(_{\text {int}}^{\mathrm {+}}\) states are measured separately for the two different areas: one area (A) along the grinded surface, and the other (B) along the original wafer surface crossing through the 57Fe-deposition boundary. By integrating the mapping intensity the diffusivity of each Fe component along the two different directions can be evaluated and compared with an average Fe diffusivity in Si, which is measured by EDS mapping data obtained for the same area. 相似文献
20.
A. W. K. Mok K. J. Sebastian 《The European Physical Journal C - Particles and Fields》2010,67(1-2):125-141
Using the helicity formalism, we calculate the combined angular distribution functions of the polarized gamma photons and electron in the triple cascade process $\bar{\mathrm{p}}\mathrm{p}\to{}^{3}\mathrm{D}_{\mathrm{2}}\to\chi_{\mathrm{\mathrm{{J}}}}+\gamma_{\mathrm{1}}\to(\psi +\gamma_{\mathrm{2}})+\gamma_{\mathrm{1}}\to(\mathrm{e}^{+}+\mathrm{e}^{-})+\gamma_{\mathrm{1}}+\gamma_{\mathrm{2}}\ (\mathrm{{J}}=0,1,2)$ , when $\bar{\mathrm{p}}$ and p are unpolarized. We also present the partially integrated angular distribution functions in different cases. Our results show that by measuring the two-particle angular distribution of γ 1 and γ 2 and that of γ 2 and e? with the polarization of either one of the two particles, one can determine the relative magnitudes as well as the relative phases of all the helicity amplitudes in the two radiative decay processes 3D2→χ J+γ 1 and χ J→ψ+γ 2. 相似文献
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