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Positive and Negative Particle Masses in the Bicubic Equation Limiting Particle Velocity Formalism

机译:限制粒子速度形式主义的双三次方程中的正负粒子质量

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The interest in the negative particle mass here got encouraged by the Rachel Gaal July 2017 APS article (Gaal, 2017) describing Khamehchi et al. (2007) observation of an effective negative mass in a spin-orbit coupled Bose-Einstein condensate. Hence, since in the bicubic equation limiting particle velocity formalism (Soln, 2014, 2015, 2016, 2017) positive m+ = m ? 0 and negative m? = ?m ? 0 masses with m2+ = m2? = m2 are equally acceptable, then from a purely theoretical point of view, the evaluation of particle limiting velocities for both m+ and a m? masses should be done. Starting with the original solutions for particle limiting velocities c1; c2 and c3, given basically for a positive particle mass m+ (Soln, 2014, 2015, 2016, 2017), now also are done for a negative particle mass m? This is done consistent with the bicubic equation mathematics, by solving for c1; c2 and c3 not only form+ but also for m?. Hence, in addition to having the limiting velocities of positive mass m+ primary, obscure and normal particles, now one has also the limiting velocities of negative mass m? primary, obscure and normal particles, however, numerically equal to limiting velocities, respectively of m+ masses obscure, primary and normal particles, forming the m+ and m? masses of equal limiting velocity value doublets : c1(m?) = c2(m+), c2(m?) = c1(m+) , c3(m?) = c3(m+). Now, one would like to know as to which particle with a negative mass m? = ?m ? 0, obtained from the positive mass m+ = m ? 0 with the substitution m ?? ?m, can have a real limiting velocity? It turns out that it is the obscure particle limiting velocity c2(m+) that changes from the imaginary value, c22(m+) ? 0, into the real limiting velocity value c22(m?) ? 0 when the change m+ ?? m? is made and, at the same time, retaining the same energy. Similar procedure applied to the original primary particle limiting velocity starting with c21(m+) ? 0 , keeping the total energy the same,with the change m ?? ?m one ends up with c21 (m?) ? 0 that is, imaginary c1. The procedure of changing m+ ?? m? in normal particle limiting velocity causes no change, it remains the same realc3. Because m2 (= m2+ = m2?), E2 and v2 remain the same , these mass regenerations, m+ ?? m? and m? ?? m+ could in principle also occur spontaneously.
机译:Rachel Gaal在2017年7月的APS文章(Gaal,2017)中描述了Khamehchi等人的观点,引起了人们对负粒子质量的兴趣。 (2007年)观察到自旋轨道耦合玻色-爱因斯坦凝聚物中的有效负质量。因此,由于在双三次方程式中限制了粒子速度的形式主义(Soln,2014、2015、2016、2017),正m + = m? 0和负m? =?m 0质量等于m2 + = m2? = m 2是同样可以接受的,那么从纯粹的理论观点来看,对于m +和m 2的颗粒极限速度的评估。群众应该做好。从原始的粒子极限速度解c1开始;基本上给定正粒子质量m +(Soln,2014,2015,2016,2017)的c2和c3,现在也针对负粒子质量m?通过求解c1可以做到与双三次方程组数学一致。 c2和c3不仅形成+,而且形成m?。因此,除了具有正质量m +初级,模糊和正常粒子的极限速度之外,现在还具有负质量m 1的极限速度。但是,初级,模糊和正常粒子在数值上分别等于m +质量模糊,初级和正常粒子的极限速度,从而形成m +和m?。极限速度值相等的质量成倍增加:c1(m1)= c2(m +),c2(m2)= c1(m +),c3(m2)= c3(m +)。现在,人们想知道哪个负质量m的粒子? =?m由正质量m + = m?0得出。 0代入m ?? ?m,可以有一个实际的极限速度吗?事实证明,是模糊的粒子极限速度c2(m +)从假想值c22(m +)改变。 0,成为实际极限速度值c22(m) 0时改变m + ??米?并同时保留相同的能量。从c21(m +)?开始,类似的程序应用于原始的一次粒子极限速度? 0,保持总能量不变,变化为m ??。 m以c21(m?)结尾吗? 0,即虚数c1。更改m + ??的过程米?在正常的粒子极限速度下不会引起任何变化,它保持不变。因为m2(= m2 + = m2?),E2和v2保持相同,所以这些质量再生m +Δω米?和米? ?? m +原则上也可以自发出现。

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