254 research outputs found

    Some clinical aspects of rheumatoid arthritis

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    In our department we have been placing a special emphasis on the treatment and study of rheumatoid arthritis, and during the last four years we have handled about 1,600 cases visiting our outpatient clinic and approximately 100 hospitalized cases. Our experiences with these patients are only what might be called an introductory phase in the study and treatment of rheumatoid arthritis when compared with those in Europe and America. In estimating the incidence of rheumatoid arthritis in Japan from various available data, although it would not reach the level of England and U.S.A., it will be about 100 cases per 100,000 population, matching more or less the incidence in the northern Europe. As regards sex and the predisposing age we find no great difference from those in Europe and America. One striking difference that we find is the fact that patients in our country have very little resistance against salicylic acid drug used in treatment. Therefore, it is unreasonable to expect a good anti-inflammatory action by administering a large dosage of 5-10g of such a drug as aspirin per day. It must be limited within a comparatively small dosage of 1.0 to 2.0 g or with concomitant administration of prednisolone and aspirin in the hope of utilizing its analgesic effect. Furthermore, it is not feasible to introduce the results of studies made in Europe and America on the salicylic drug and its prescription all of them showing the concentration in blood 35 mg%, which is on the borderline of intoxicating dosage. This is only one example, and with some more experiences we shall undoubtedly encounter many dissimilar points. Therefore, it is essential that rheumatology specific to Japan needs to be established.</p

    Redshift Dependent Lag-Luminosity Relation in 565 BASTE Gamma Ray Bursts

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    We compared redshifts zYz_Y from Yonetoku relation and zlagz_{lag} from the lag-luminosity relation for 565 BASTE GRBs and were surprised to find that the correlation is very low. Assuming that the luminosity is a function of both zYz_Y and the intrinsic spectral lag Ο„lag\tau_{lag}, we found a new redshift dependent lag-luminosity relation as L=7.5Γ—1050erg/s(1+z)2.53Ο„lagβˆ’0.282L=7.5\times 10^{50}{\rm erg/s}(1+z)^{2.53}\tau_{lag}^{-0.282} with the correlation coefficient of 0.77 and the chance probability of 7.9Γ—10βˆ’757.9\times 10^{-75}. To check the validity of this method, we examined the other luminosity indicator, Amati relation, using zYz_Y and the observed fluence and found the correlation coefficient of 0.92 and the chance probability of 5.2Γ—10βˆ’1065.2\times 10^{-106}. Although the spectral lag is computed from two channels of BATSE, our new lag-luminosity relation suggests that a possible lag-luminosity relation in the \swift era should also depend on redshift

    Constraints on w0w_0 and waw_a of Dark Energy from High Redshift Gamma Ray Bursts

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    We extend the Hubble diagram up to z=5.6z = 5.6 using 63 gamma-ray bursts (GRBs) via peak energy-peak luminosity relation (so called Yonetoku relation), and obtain constraints on cosmological parameters including dynamical dark energy parametrized by P/ρ≑w(z)=w0+waβ‹…z/(1+z)P/\rho\equiv w(z) = w_0 + w_a \cdot z/(1+z). It is found that the current GRB data are consistent with the concordance model, (Ξ©m=0.28,ΩΛ=0.72,w0=βˆ’1,wa=0\Omega_m = 0.28, \Omega_{\Lambda} = 0.72, w_0 = -1, w_a = 0), within two sigma level. Although constraints from GRBs themselves are not so strong, they can improve the conventional constraints from SNeIa because GRBs have much higher redshifts. Further we estimate the constraints on the dark-energy parameters expected by future observations with GLAST (Gamma-ray Large Area Space Telescope) and \swift by Monte-Carlo simulation. Constraints would improve substantially with another 150 GRBs.Comment: 5 pages, 6 figures. Submitted tu MNRA

    Gamma-Ray Bursts in 1.8<z<5.61.8 < z < 5.6 Suggest that the Time Variation of the Dark Energy is Small

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    We calibrated the peak energy-peak luminosity relation of GRBs (so called Yonetoku relation) using 33 events with the redshift z<1.62z < 1.62 without assuming any cosmological models. The luminosity distances to GRBs are estimated from those of large amount of Type Ia supernovae with z<1.755z<1.755. This calibrated Yonetoku relation can be used as a new cosmic distance ladder toward higher redshifts. We determined the luminosity distances of 30 GRBs in 1.8<z<5.61.8 < z < 5.6 using the calibrated relation and plotted the likelihood contour in (Ξ©m,ΩΛ)(\Omega_m,\Omega_\Lambda) plane. We obtained (Ξ©m,ΩΛ)=(0.37βˆ’0.11+0.14,0.63βˆ’0.14+0.11)(\Omega_m, \Omega_{\Lambda})= (0.37^{+0.14}_{-0.11}, 0.63^{+0.11}_{-0.14}) for a flat universe. Since our method is free from the circularity problem, we can say that our universe in 1.8<z<5.61.8 < z < 5.6 is compatible with the so called concordance cosmological model derived for z<1.8z < 1.8. This suggests that the time variation of the dark energy is small or zero up to z∼6z\sim 6.Comment: 4 pages, 4 figures, accepted to MNRA

    Cosmological Constraints from calibrated Yonetoku and Amati relation implies Fundamental plane of Gamma-ray bursts

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    We consider two empirical relations using data only from the prompt emission of Gamma-Ray Bursts (GRBs), peak energy (EpE_p) - peak luminosity (LpL_p) relation (so called Yonetoku relation) and EpE_p-isotropic energy (EisoE_{\rm iso}) relation (so called Amati relation). We first suggest the independence of the two relations although they have been considered similar and dependent. From this viewpoint, we compare constraints on cosmological parameters, Ξ©m\Omega_m and ΩΛ\Omega_{\Lambda}, from the Yonetoku and Amati relations calibrated by low-redshift GRBs with z<1.8z < 1.8. We found that they are different in 1-Οƒ\sigma level, although they are still consistent in 2-Οƒ\sigma level. This and the fact that both Amati and Yonetoku relations have systematic errors larger than statistical errors suggest the existence of a hidden parameter of GRBs. We introduce the luminosity time TLT_L defined by TL≑Eiso/LpT_L\equiv E_{\rm iso}/L_p as a hidden parameter to obtain a generalized Yonetoku relation as (Lp/1052ergsβˆ’1)=10βˆ’3.88Β±0.09(Ep/keV)1.84Β±0.04(TL/s)βˆ’0.34Β±0.04(L_p/{10^{52} \rm{erg s^{-1}}}) = 10^{-3.88\pm0.09}(E_p/{\rm{keV}})^{1.84\pm0.04} (T_L/{\rm{s}})^{-0.34\pm0.04}. The new relation has much smaller systematic error, 30%, and can be regarded as "Fundamental plane" of GRBs. We show a possible radiation model for this new relation. Finally we apply the new relation for high-redshift GRBs with 1.8<z<5.61.8 < z < 5.6 to obtain (Ξ©m,ΩΛ)=(0.16βˆ’0.06+0.04,1.20βˆ’0.09+0.03)(\Omega_m,\Omega_{\Lambda}) = (0.16^{+0.04}_{-0.06},1.20^{+0.03}_{-0.09}), which is consistent with the concordance cosmological model within 2-Οƒ\sigma level.Comment: 5 pages, 6 figures, published in JCA
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