Javascript must be enabled to continue!
A Low Energy Clock Network with a Huge Number of Local Synchronized Oscillators
View through CrossRef
<p>Manycore processors may generally be implemented as an array of small processing elements (PE) interconnected by a communication mesh (NoC). This article describes a clock system for such chips, with many thousands of high frequency PEs.</p>
<p>Each PE contains a low energy oscillator. It synchronizes with the four neighbors by an additional low voltage wire parallel to the communication links, which carries a sinusoidal signal. This wire is part of a resonant circuit that extends to all PE oscillators. Theoretically, in an infinite mesh the oscillators will all be phase locked, but in a limited mesh there will be fringe effects. In a mesh with 25×25 oscillators, the maximum skew between neighboring regions is within 3.3 ps. By slightly adjusting the free running frequency of the oscillators, the skew can be reduced to 1.2 ps.</p>
<p>Because there is no central clock, both power consumption and clock frequency can be improved compared to a conventional clock distribution network. A PE of 150×150 μm² running at 6.7 GHz with 93 master-slave flip-flops is used as an example. The PE-internal clock skew is less than 2.3 ps, and the energy consumption of the clock system 807 μW per PE. This corresponds to an effective gate and wire capacitance of 509 aF, or 7.3 gate capacitances.</p>
<p>Scheduling the local oscillators gradually along one of the grid’s axes reduces the power noise. In this way, surge currents, which generally have their peaks at the clock edges, are distributed evenly over a full clock cycle.</p>
Title: A Low Energy Clock Network with a Huge Number of Local Synchronized Oscillators
Description:
<p>Manycore processors may generally be implemented as an array of small processing elements (PE) interconnected by a communication mesh (NoC).
This article describes a clock system for such chips, with many thousands of high frequency PEs.
</p>
<p>Each PE contains a low energy oscillator.
It synchronizes with the four neighbors by an additional low voltage wire parallel to the communication links, which carries a sinusoidal signal.
This wire is part of a resonant circuit that extends to all PE oscillators.
Theoretically, in an infinite mesh the oscillators will all be phase locked, but in a limited mesh there will be fringe effects.
In a mesh with 25×25 oscillators, the maximum skew between neighboring regions is within 3.
3 ps.
By slightly adjusting the free running frequency of the oscillators, the skew can be reduced to 1.
2 ps.
</p>
<p>Because there is no central clock, both power consumption and clock frequency can be improved compared to a conventional clock distribution network.
A PE of 150×150 μm² running at 6.
7 GHz with 93 master-slave flip-flops is used as an example.
The PE-internal clock skew is less than 2.
3 ps, and the energy consumption of the clock system 807 μW per PE.
This corresponds to an effective gate and wire capacitance of 509 aF, or 7.
3 gate capacitances.
</p>
<p>Scheduling the local oscillators gradually along one of the grid’s axes reduces the power noise.
In this way, surge currents, which generally have their peaks at the clock edges, are distributed evenly over a full clock cycle.
</p>.
Related Results
A Low Energy Clock Network with a Huge Number of Local Synchronized Oscillators
A Low Energy Clock Network with a Huge Number of Local Synchronized Oscillators
<div>A clock system for a huge grid of small clock regions is presented. There is an oscillator in each clock region, which drives the local clock of a processing element (PE...
A Low Energy Clock Network with a Huge Number of Local Synchronized Oscillators
A Low Energy Clock Network with a Huge Number of Local Synchronized Oscillators
<p>Manycore processors may generally be implemented as an array of small processing elements (PE) interconnected by a communication mesh (NoC). This article describes a clock...
Solving Undamped and Damped Fractional Oscillators via Integral Rohit Transform
Solving Undamped and Damped Fractional Oscillators via Integral Rohit Transform
Background: The dynamics of fractional oscillators are generally described by fractional differential equations, which include the fractional derivative of the Caputo or Riemann-Li...
Nonlinear simulation and design of microwave, multi-device distributed autonomous circuits
Nonlinear simulation and design of microwave, multi-device distributed autonomous circuits
It is widely believed that many drawbacks in today's wireless communication paradigm might be relieved by enabling high carrier frequency transmission, and endowing both the networ...
Single Operational Current Amplifier Based Sinusoidal Oscillators
Single Operational Current Amplifier Based Sinusoidal Oscillators
Abstract
This paper presents important missing sinusoidal oscillators. There are numerous sinusoidal oscillators versions based on the three fundamental amplifiers namely t...
Method and Performance of Time Holdover for RT-PPT Receivers Utilizing on-line Estimation of Clock Parameters
Method and Performance of Time Holdover for RT-PPT Receivers Utilizing on-line Estimation of Clock Parameters
Abstract
Real Time Precise Point Timing (RT-PPT) receivers can achieve sub-nanosecond accuracy through precise clock offset estimation and receiver clock discipline. Howeve...
Clock Genes and Cancer
Clock Genes and Cancer
Period genes ( Per2, Per1) are essential circadian clock genes. They also function as negative growth regulators. Per2 mutant mice show de novo and radiation-induced epithelial hyp...
Feedback Oscillators
Feedback Oscillators
AbstractIn this article, the basic theory of feedback oscillators related to balanced condition, startup condition, stability condition, frequency stability, and other characterist...

