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Prospects for measuring the moment of inertia of pulsar J0737-3039A

机译:测量脉冲星J0737-3039A惯性矩的前景

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Here we consider the possibility-envisaged by many authors as feasible in the near future-of measuring at 10% or better the moment of inertia / of the pulsar J0737-3039A via the gravitomagnetic spin-orbit periastron precession (analogous to the Lense-Thirring pericentre precession in the case of a test-particle orbiting a central spinning mass). Such a gravitomagnetic effect is expected to be of the order of 10 (4) deg yr (1) and the present-day precision in measuring the periastron precession of J0737-3039A via pulsar timing is 6.8 x 10 (4) deg yr (1). However the systematic uncertainty in the much larger first-order post-Newtonian (IPN) gravitoelectric precession (analogous to the Einstein Mercury's perihelion precession in the weak-field and slow-motion approximation), which should be subtracted from the measured one in order to pick up the gravitomagnetic rate, is of primary importance. Indeed, by determining the sum of the masses by means of the third Kepler law, such a bias amounts to 0.03165 deg yr (1), according to the current level of accuracy in knowing the parameters of the J0737-3039 system. The major sources of uncertainty are the Keplerian projected semimajor axis x(B) of the component B and the post-Keplerian parameters, identified with sin i; their knowledge should be improved by three orders of magnitude at least; the bias due to the Keplerian projected semimajor axis x(A) of the component A amounts to approximate to 10% today. The present-day level of accuracy in the eccentricity e would affect the investigated measurement at a percent level, while the impact of the orbital period P-b is completely negligible. If, instead, the sum of the masses is measured by means of the post-Keplerian parameters r and s, it turns out that r should be measured five orders of magnitude better than now: according to the present-day level of accuracy, the total uncertainty in the IPN periastron rate is, in this case, 2.11819 deg yr (1). In conclusion, the prospect of measuring the moment of inertia of PSR J0737-3039A at 10% accuracy or better seems unlikely given the limitations to the precision with which the system's basic binary and post-Keplerian parameters can be measure via radio timing. (C) Elsevier B.V. All rights reserved.
机译:在这里,我们认为许多作者设想的可能性在不久的将来是可行的,即通过重力自旋轨道绕星过程进动测量脉冲星J0737-3039A的转动惯量/的10%或更高(类似于Lense-Thirring)如果测试粒子绕中心旋转的质量旋转,则中心点进动。这种重力效应预计约为10(4)deg yr(1),目前通过脉冲星定时测量J0737-3039A的周星旋进的精度为6.8 x 10(4)deg yr(1)。 )。但是,更大的一阶后牛顿(IPN)重力电进动中的系统不确定性(类似于爱因斯坦水星在弱视场和慢动作逼近中的近日点进动),应从测得的误差中减去加快重力速度,是最重要的。实际上,根据第三种开普勒定律确定质量的总和,根据当前了解J0737-3039系统参数的准确度,这样的偏差为0.03165度yr(1)。不确定性的主要来源是分量B的开普勒投影半长轴x(B)和后开普勒参数,用sin i表示。他们的知识至少应提高三个数量级;今天,由分量A的开普勒投影半长轴x(A)引起的偏差大约为10%。目前偏心距e的精度水平将以百分比水平影响所研究的测量结果,而轨道周期P-b的影响则可以忽略不计。取而代之的是,如果通过后开普勒参数r和s测量质量的总和,则结果表明r的测量应比现在好五个数量级:根据当今的精确度,在这种情况下,IPN围发性心律失常率的总不确定度为2.11819度yr(1)。总之,鉴于可以通过无线电计时来测量系统基本二进制和后基普勒参数的精度受到限制,因此以10%或更高的精度测量PSR J0737-3039A的惯性矩的可能性似乎很小。 (C)Elsevier B.V.保留所有权利。

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