用离散相关函数方法分析Blazar天体的γ射线和射电辐射的相关性

收集了119颗有γ射线噪的Blazar天体样品(97个平谱射电类星体和22个BL Lac天体)，用离散相关函数(DCF)方法分析了1GeV γ射线辐射流量(最大值、最小值和平均值)与8.4GHz射电辐射流量之间的相关性.获得的主要结果为：在119个Blazar天体和97个平谱射电类星体中，γ射线辐射流量的最大值以及平均值和射电辐射流量之间有相关性;而γ射线辐射流量的最小值和射电辐射流量之间没有相关性.本文结果表明，γ射线和射电辐射都来自喷流，γ射线很可能产生于同步自康普顿(SSC)过程. 关键词： Blazar γ射线 射电辐射 流量密度     

BL Lac天体的γ射线和射电辐射的统计特性

给出了一个带有射电5.0GHz,8.4GHz 和γ射线辐射流量密度的22个γ噪BL Lac天体的样本,研究了它们在1GeV处的γ射线辐射流量密度最大值、平均值及最小值与射电5.0GHz,8.4GHz辐射流量之间的可能关系.结果表明：1）射电5.0GHz,8.4GHz辐射与γ射线辐射在低态时没有相关,但在高态和平均态时都存在较强的相关,最大相关系数r=0.85,置信度均好于10^-4;2）γ射线谱指数和射电谱指数之间也有一个弱相关关系存在.因此,认为γ射线的辐射主要是同步自康普顿辐射. 关键词： BL Lac天体 γ射线 射电辐射 谱指数     

Blazar天体的光变和偏振

从已有文献中收集了一定数量的有关Blazar天体的数据，分析光变、偏振度以及核优参数之间的相关性，结果表明光变和偏振及核优参数之间有一定的关系，这可能暗示Blazar天体存在着聚束效应. 关键词： Blazar天体 光变幅度 偏振度 核优参数     

基于Logistic回归模型的Blazar天体的分类

从文献中收集了205个Blazar天体,包括142个BL Lac天体和63个平谱射电类星体(FSRQs).对这些天体的类别与它们的红移、射电5 GHz辐射流量、光学V波段流量、1 keV处X射线流量、X射线光子谱指数进行了相关性和Logistic回归分析.结果表明,对Blazar天体分类产生主要影响的因素是红移、射电5 GHz辐射流量和X射线光子谱指数,综合应用这三个物理量判别Blazar天体的分类的准确率可达到91.2%,得到的分类方程具有良好的预测效果,可以作为Blazar天体分类的一个重要的判据.而光学V波段流量和1 keV处X射线流量不能区分开BL Lac天体和FSRQs,它们与Blazar天体分类没有相关性.本文结果支持将BL Lac天体和FSRQs归为Blazar天体,不同类别的Blazar天体之间能通过一种演化序列相联系. 关键词： Logistic 分类 Blazar天体     

γ射线暴的最新研究进展:火球模型、余辉及前身星

γ射线暴 (称简γ暴 )的研究在最近几年里有了巨大的突破。观测上 ,人们发现了γ暴的低能余辉以及与γ射线爆发同时的光学爆发 ,还发现了它位于宇宙学距离的寄主星系。越来越多的观测证据还表明长时标γ暴与恒星形成区、甚至可能与超新星成协。在γ暴的相对论火球模型框架下 ,人们对γ暴以及余辉的产生机制的认识也有了进展。进而人们对γ暴的前身星以及环境效应等有了新的认识。本文旨在对这些进展和认识给一个扼要的评述     

宇宙γ射线暴

 γ射线暴(以下简称γ暴)是来自宇宙空间的一种短时标的高能γ射线爆发现象。它的发现颇有戏剧性:60年代中期,为了监督关于禁止在大气层中进行核试验的条约的执行情况,美国发射了一些卫星,以监测核爆炸中的γ射线事件。1967年开始,Ｖｅｌａ卫星真的不时记录到一些γ射线爆发现象,使美国政府十分紧张。军方花了几年的时间终于搞清楚它们均来自于宇宙空间,证实只是一场虚惊。由于军事保密的原因,该现象直到1973年才由美国洛斯阿拉莫斯实验室的Ｋｌｅｂｅｓａｄｅｌ、Ｓｔｒｏｎｇ和Ｏｌｓｏｎ在ＡｐＪ(美国《天体物理杂志》)的一篇快报中以“对源自宇宙空间的γ射线爆发的观测”为题发表出来。     

一种新型辐射变色膜的γ射线辐照研究

报道了以高聚物为载体,以有机染料及添加剂为变色指示剂体系,制备一种辐射变色膜。这种辐射变色膜为无色透明固体薄膜,经60Co γ射线辐照后,其颜色变为蓝色。辐照后样品的紫外-可见吸收光谱表明,在可见光区其最强吸收峰出现在624 nm附近。在10～90 kGy的剂量范围内,不含添加剂的辐射变色膜的光密度变化与吸收剂量呈线性关系,而含有添加剂的辐射变色膜对γ射线辐照的响应在50 kGy时就达到饱和。同时还探索了该体系辐照效应的化学反应机理。     

中重核中子辐射俘获γ射线强度函数研究

假设退激过程中除包含巨偶极共振模式外还存在⁶He,⁶Li,⁶Be,⁷Li和⁷Be等粒子集团激发态的退激过程.本文对这一物理假定作了进一步分析.利用据此建立的包括这些过程在内的γ射线强度函数,计算了在核素⁹³Nb,¹⁸¹Ta和天然元素Ag上入射中子能量在0.01—5MeV能区以及在核素¹⁹⁷Au上入射中子能量在0.01—10MeV能区的中子辐射俘获反应截面和γ能谱,得到了与实验数据较好符合的结果.特别是可以较好地解释γ能谱中5.5MeV之后的反常突起.这表明,上述物理假定适用于中重核中子辐射俘获反应.     

γ暴研究的重大突破：首次观测到γ暴的光学和X射线余辉

意大利和荷兰联合发射的卫星ＢｅｐｐｏＳＡＸ在１９９７年２月２８日探测到γ暴ＧＲＢ９７０２２８的Ｘ射线余辉，随后的地面和哈勃空间望远镜的观测证实在该位置上有一光学瞬变源。哈勃空间望远镜在此光学变源方位观测到一暗的河外天体。     

γ射线弹和射线防护

 1896年,法国物理学家贝克勒尔发现铀具有放射性,能不断放射出一种肉眼看不见而穿透本领很强的射线。后来,科学家经过研究发现放射线是由3种很强的射线组成的:一种是α射线(氦核),另一种是β射线(电子),还有一种是γ射线(光子)。此后,放射线在包括军事领域在内的多方面得到应用。最近,继第三代核武器中子弹研制成功后,一些军事强国又把目光投向了另一种核武器———γ射线弹,使全世界爱好和平的人们心头蒙上了一层新的核阴影。一、γ射线弹一般来说,核爆炸的杀伤力量由4个因素组成:冲击波、光辐射、放射性沾染和贯穿辐射,其中贯穿辐射主要由强γ射线和中子流组成。     

GAMMA-RAY AND X-RAY EMISSION FROM GAMMA-RAY-LOUD BLAZARS

We present a strong correlation of the gamma-ray (above 100 MeV) mean spectral indices α_γ and X-ray (1 keV) mean spectral indices α_X for 34 gamma-ray-loud blazars (16 BL Lac objects and 18 flat spectrum radio quasars). A strong correlation is also found between the gamma-ray flux densities F_γ and X-ray flux densities F_X in the low state for 47 blazars (17 BL Lac and 30 flat spectrum radio quasars). Possible correlation on the gamma-ray emission mechanism is discussed. We suggest that the main gamma-ray radiation mechanism is probably the synchrotron process. The gamma-ray emission may be somewhat different from that of BL Lac objects and flat spectrum radio quasars.     

TeV gamma rays from distant BL Lacs and photon–paraphoton kinetic mixing

An effect of a proposed Beyond the Standard Model particle physics process on the energy spectra of distant astrophysical objects is presented. It is suggested that TeV gamma rays from distant BL Lacs may kinetically mix with hypothetical hidden sector paraphotons. The latter can traverse vast distances of space because of only very weak interactions with intervening objects or material. These paraphotons would then reconvert back into photons that have identical characteristics as their originators, and are detected on earth. Laser based photon regeneration experiments test this model of hidden sector physics in the range of parameters that would impact the TeV gamma ray energy spectra arriving from distant BL Lacs.     

Central black hole mass determination for blazars

In this paper, we use a method to determine some basic parameters for the $\gamma$-ray loud blazars. The parameters include the central black mass ($M$), the boosting factor ($\delta$), the propagation angle (${\it {\it\Phi}}$), the distance along the axis to the site of the $\gamma$-ray production ($d$). A sample including 32 $\gamma$-ray loud blazars with available variability time scales has been used to discuss the above properties. In this method, the $\gamma$-ray energy, the emission size and the property of the accretion disc determine the absorption effect. If we take the intrinsic $\gamma$-ray luminosity to be $\lambda$ times the Eddington luminosity, i.e. $L_{\gamma}^{\rm in}=\lambda{L_{\rm Edd}}$, then we have the following results: the mass of the black hole is in the range of $(0.59-67.99)\times10^{7}M_{\odot} \ (\lambda=1.0)$ or $(0.90-104.13)\times10^{7}M_{\odot} \ (\lambda=0.1)$; the boosting factor ($\delta$) in the range of In this paper, we use a method to determine some basic parameters for the $\gamma$-ray loud blazars. The parameters include the central black mass ($M$), the boosting factor ($\delta$), the propagation angle (${\it {\it\Phi}}$), the distance along the axis to the site of the $\gamma$-ray production ($d$). A sample including 32 $\gamma$-ray loud blazars with available variability time scales has been used to discuss the above properties. In this method, the $\gamma$-ray energy, the emission size and the property of the accretion disc determine the absorption effect. If we take the intrinsic $\gamma$-ray luminosity to be $\lambda$ times the Eddington luminosity, i.e. $L_{\gamma}^{\rm in}=\lambda{L_{\rm Edd}}$, then we have the following results: the mass of the black hole is in the range of $(0.59-67.99)\times10^{7}M_{\odot} \ (\lambda=1.0)$ or $(0.90-104.13)\times10^{7}M_{\odot} \ (\lambda=0.1)$; the boosting factor ($\delta$) in the range of In this paper, we use a method to determine some basic parameters for the $\gamma$-ray loud blazars. The parameters include the central black mass ($M$), the boosting factor ($\delta$), the propagation angle (${\it {\it\Phi}}$), the distance along the axis to the site of the $\gamma$-ray production ($d$). A sample including 32 $\gamma$-ray loud blazars with available variability time scales has been used to discuss the above properties. In this method, the $\gamma$-ray energy, the emission size and the property of the accretion disc determine the absorption effect. If we take the intrinsic $\gamma$-ray luminosity to be $\lambda$ times the Eddington luminosity, i.e. $L_{\gamma}^{\rm in}=\lambda{L_{\rm Edd}}$, then we have the following results: the mass of the black hole is in the range of $(0.59-67.99)\times10^{7}M_{\odot} \ (\lambda=1.0)$ or $(0.90-104.13)\times10^{7}M_{\odot} \ (\lambda=0.1)$; the boosting factor ($\delta$) in the range of In this paper, we use a method to determine some basic parameters for the $\gamma$-ray loud blazars. The parameters include the central black mass ($M$), the boosting factor ($\delta$), the propagation angle (${\it {\it\Phi}}$), the distance along the axis to the site of the $\gamma$-ray production ($d$). A sample including 32 $\gamma$-ray loud blazars with available variability time scales has been used to discuss the above properties. In this method, the $\gamma$-ray energy, the emission size and the property of the accretion disc determine the absorption effect. If we take the intrinsic $\gamma$-ray luminosity to be $\lambda$ times the Eddington luminosity, i.e. $L_{\gamma}^{\rm in}=\lambda{L_{\rm Edd}}$, then we have the following results: the mass of the black hole is in the range of $(0.59-67.99)\times10^{7}M_{\odot} \ (\lambda=1.0)$ or $(0.90-104.13)\times10^{7}M_{\odot} \ (\lambda=0.1)$; the boosting factor ($\delta$) in the range of In this paper, we use a method to determine some basic parameters for the $\gamma$-ray loud blazars. The parameters include the central black mass ($M$), the boosting factor ($\delta$), the propagation angle (${\it {\it\Phi}}$), the distance along the axis to the site of the $\gamma$-ray production ($d$). A sample including 32 $\gamma$-ray loud blazars with available variability time scales has been used to discuss the above properties. In this method, the $\gamma$-ray energy, the emission size and the property of the accretion disc determine the absorption effect. If we take the intrinsic $\gamma$-ray luminosity to be $\lambda$ times the Eddington luminosity, i.e. $L_{\gamma}^{\rm in}=\lambda{L_{\rm Edd}}$, then we have the following results: the mass of the black hole is in the range of $(0.59-67.99)\times10^{7}M_{\odot} \ (\lambda=1.0)$ or $(0.90-104.13)\times10^{7}M_{\odot} \ (\lambda=0.1)$; the boosting factor ($\delta$) in the range of $0.16-2.09(\lambda=1.0)$ or $0.24-2.86\ (\lambda=0.1)$; the angle (${\it\Phi}$) in the range of $9.53^{\circ}-73.85^{\circ}\ (\lambda=1.0)$ or $7.36^{\circ}-68.89^{\circ}\ (\lambda=0.1)$; and the distance ($d/R_{\rm g}$) in the range of $22.39-609.36\ (\lambda=1.0)$ or $17.54-541.88\ (\lambda=0.1)$.     

Mkn 501 X射线和TeV射线准周期震荡的可能机制

我们提出了对流占主导的吸积流（ADAF）盘的辐射线是Mkn 501中从X射线到Tevγ射线的源光子；而且此盘的不稳定性可以解释Mkn 501中在X射线和Tevγ射线光变曲线23天的准周期光变。在这个模型中,光学到X射线辐射进入喷流，后由于喷流内相对论电子的作用而转化成高能光子。在这个过程中，发生在ADAF盘中的不稳定性导致源光子的准周期变化，从而导致了X射线和γ射线的变化。     

Statistical properties of extragalactic radio sources

In this paper, a large sample of extragalactic radio sources is analysed to show their statistical properties. The core and total radio powers are used to determine the core-dominance parameter for galaxies, BL Lacertae objects and quasars; mutual correlations between core radio power, total radio power, redshift and core dominance parameter are examined for different subclasses. A statistically significant correlation between the total and core radio power is confirmed. There are no obvious correlations between core-dominance parameter and the total power for our whole sample and quasars, but there is a statistically significant anti-correlation for our galaxy sample. Some discussions and comparison of the correlations with those obtained by other authors are also given.     

THE DIFFERENCE OF OPTICAL POLARIZATION PROPERTIES BETWEEN XBLs AND RBLs

On the basis of the beaming model, we have derived a relation between the observed polarization (P^ob) and Doppler-corrected optical magnitude (m^corr), log P^ob=0.4(1-k) m^corr+C. We tested the correlation between P^{ob} and mcorr. The main results are as follows: (1) for both high and low states, there are strong correlations between Pob and mcorr for 29 RBLs with well-observed polarization and Doppler factor, where mcorr=mob+(3+α)logδ/0.4, and δ is the optical Doppler factor; (2) no correlation exists between Pob and the observed optical magnitude, mob, for the 29 RBLs in high state, but there is a close correlation for the 29 RBLs in low state; (3) however, there is an obvious anti-correlation between Pob and mcorr for 35 XBLs with good simultaneous observation data. Our results show that (i) a new difference in polarization is found between RBLs and XBLs; (ii) this difference in polarization between RBLs and XBLs seems really to be physical differences.}     

SPECTRAL VARIABILITY AND TRANSIENT INJECTION OF RELATIVISTIC ELECTRONS FOR BL LAC OBJECTS

The spectral hardening with increasing intensity in optical range for four BL Lac objects have been found by analyzing our observed data. Making use of the synchrotron loss of transient injection of relativistic electrons, we succeeded in explaining the phenomenon of the spectral hardening in the outburst phase. The value of magnetic intensity and the limit condition of the transient injection of relativistic electrons seem to be reasonable.     

柴油机醛酮污染物排放规律的试验研究

采用DNPH衍生法和液相色谱(HPLC)技术对生物柴油发动机排气中的羰基化合物(醛、酮)进行了捕集和分离测定,通过燃用BD100,BD50,BDO三种不同调合比例的生物柴油,测量了标定转速,不同负荷下的醛、酮污染物.在此基础上,分析了燃料组分、燃烧参数、排气温度等因素对醛、酮污染物排放的影响.结果表明,根据衍生剂与羰基...     

用场发射显微镜研究单壁碳纳米管场发射

利用场发射显微镜在小于40×10^-7Pa压强条件下研究了单壁碳纳米管微束在不同温度加热除气后的场发射变化,得出随着除气温度的升高,碳纳米管逸出功经历了从大到小再变大的变化过程.在清洁态(1000℃除气)对应有最小的逸出功,此时场发射图像显示出一定的细致结构.继续升高温度,碳纳米管发生塌缩.     

润滑剂分子结构及其润滑作用机理的红外发射光谱研究

在自制的“原位“摩擦装置上,利用红外发射光谱技术对润滑剂在摩擦过程中的化学行为进行跟踪测量,以期对润滑剂分子结构变化与润滑作用机理进行某些关联。实验证明,红外发射光谱技术可作为原位观测摩擦过程中化学变化的有效手段。