异构业务系统中速度感知JSQ的渐近最优性

Sanidhay Bhambay, Arpan Mukhopadhyay
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引用次数: 4

摘要

众所周知,加入最短队列(JSQ)负载平衡方案可以最小化由相同服务器组成的同构系统中作业的平均延迟。但是,在服务器具有不同处理速率的异构系统中,它的性能很差。对于异构系统,寻找延迟最优方案一直是一个有待解决的问题。在本文中,我们考虑了异构系统的JSQ方案的速度感知版本,并证明了它在流体限制下实现了延迟最优性。建立异构系统最优性结果的关键问题之一是证明由系统大小索引的稳态分布序列在适当定义的空间内是紧密的。通常通过与适当定义的主导系统耦合来显示紧密性的技术不适用于异构系统。为了证明紧密性,我们设计了一种利用指数李雅普诺夫函数漂移的新技术。利用漂移的非负性,我们证明了平稳队列长度分布有一个指数衰减的尾部——这是我们用来证明紧密性的事实。另一个技术困难是由于底层状态空间的复杂性和流体极限中两个时间尺度的分离。由于这些因素,流体极限变成了多维马尔可夫链不变分布的函数,难以表征。利用该不变量分布的一些性质,利用系统的单调性,证明了流体极限具有唯一且全局吸引的不动点。
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Asymptotic optimality of speed-aware JSQ for heterogeneous service systems
The Join-the-Shortest-Queue (JSQ) load-balancing scheme is known to minimise the average delay of jobs in homogeneous systems consisting of identical servers. However, it performs poorly in heterogeneous systems where servers have different processing rates. Finding a delay optimal scheme remains an open problem for heterogeneous systems. In this paper, we consider a speed-aware version of the JSQ scheme for heterogeneous systems and show that it achieves delay optimality in the fluid limit. One of the key issues in establishing this optimality result for heterogeneous systems is to show that the sequence of steady-state distributions indexed by the system size is tight in an appropriately defined space. The usual technique for showing tightness by coupling with a suitably defined dominant system does not work for heterogeneous systems. To prove tightness, we devise a new technique that uses the drift of exponential Lyapunov functions. Using the non-negativity of the drift, we show that the stationary queue length distribution has an exponentially decaying tail - a fact we use to prove tightness. Another technical difficulty arises due to the complexity of the underlying state-space and the separation of two time-scales in the fluid limit. Due to these factors, the fluid-limit turns out to be a function of the invariant distribution of a multi-dimensional Markov chain which is hard to characterise. By using some properties of this invariant distribution and using the monotonicity of the system, we show that the fluid limit is has a unique and globally attractive fixed point.
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