Open Quantum Systems
开源云平台和OpenStack介绍

源码
完全开源
完全开源
完全开源
完全开源
开发模式 Internet公开 Internet公开 Internet公开 Internet公开
开发约束 Apache v2.0 Apache v2.0 GPL v3.0
Apache v2.0
管理模式 基金会
技术精英
仁慈的独裁者 仁慈的独裁者
API生态系统 OpenStack API Amazon API Amazon API Amazon API
More complex to set up. Compute nodes typically need IP addresses accessible by external networks. Options must be carefully configured for live migration to work with networking services.
OpenStack与其它开源技术 消息队列 数据库 Web服务器 HA
操作系统
corosync
Openstack支持的Hypervisor
https:///wiki/HypervisorSupportMatrix
OpenStack安装 官方推荐安装的Linux发行版
产品可用性
需要定制开发 企业级,由社 企业级,由社 企业级,由社
或者由厂家支 区开发者直接 区开发者直接 区开发者直接
持
支持
支持
支持
主要开发语言 Python
Java&Python Java&C/C++ Ruby
社区活跃度
社区人员总数
活跃社区人数
OpenStack介绍
open quantum materials database的使用方法

open quantum materials database的使用方法【原创版】目录1.Open Quantum Materials Database 简介2.数据库的结构和内容3.使用方法:搜索、浏览和下载数据4.应用案例和注意事项5.结论正文1.Open Quantum Materials Database 简介Open Quantum Materials Database(OQMD)是一个免费的在线数据库,旨在为科研人员提供关于量子材料的实验和理论数据。
这个数据库包含了大量关于量子材料的信息,如电子结构、光学性质、磁性等,为广大科研工作者提供了宝贵的资源。
2.数据库的结构和内容OQMD 数据库采用了模块化的结构,用户可以根据需要浏览和搜索不同模块的数据。
目前,数据库主要包括以下几个模块:(1)材料属性:包括晶体结构、空间群、原子坐标等基本信息;(2)电子结构:包括带隙、态密度、费米面等;(3)光学性质:包括吸收系数、折射率、光谱等;(4)磁性:包括磁化率、磁矩、磁导率等;(5)其他:如热学、电学等性质。
3.使用方法:搜索、浏览和下载数据(1)搜索数据:用户可以通过关键词搜索、材料名称搜索或物质编号搜索等方式,快速找到所需数据。
搜索结果会以列表形式展示,包括材料名称、属性名称和具体数值等。
(2)浏览数据:用户可以按照模块浏览数据,了解各个模块的具体内容。
同时,也可以通过分类和排序功能,更加方便地查找和比较数据。
(3)下载数据:用户可以选择需要的数据,点击“下载”按钮将其导出为 CSV、XLSX 等格式文件。
下载的数据可以用于进一步的分析和处理。
4.应用案例和注意事项(1)应用案例:OQMD 数据库的数据可以广泛应用于量子材料的研究、设计和应用等领域。
例如,研究人员可以通过比较不同材料的电子结构,寻找具有特定性能的材料;也可以通过分析材料的光学性质,优化器件的性能等。
(2)注意事项:在使用数据库时,请注意遵守相关法律法规和知识产权保护政策。
CANopen协议应用指南

Protocol Layer Interactions
协议层交互
发送设备
CANopen Application
Layer
CAN Data Link Layer
CAN Physical Layer
Object at Index
ID + Data ... ID + data
CAN_L CAN_H CAN_L
Mini Style Connector
5-pin Mini Style Connector : ANSI/B93.55M-1981
male 3
female 3
4
22
4
5
11
5
If 5-pin Mini Style Connectors are used the following pinning applies:
Data Link Layer and High-Speed Transceiver (ISO 11898)
BBiti-t-TTimimininggaannddCCoonnnneecctotorrPPinin--AAssssigignnmmeenntt
bus lines
Ó CiA
CANopen通讯概念可以类似ISO Open Systems Interconnection (OSI) Reference Model描述. CANopen描述了一种标准化应用层和通讯协议。用于可编程设备的可选框架规定了额外的通讯功 能。
Open Style Connector
Open Style Connector
female
male 12345
123 4 5
If Open Style Connectors are used the following pinning is recommended:
非厄米算符对易关系

非厄米算符对易关系Quantum mechanics plays a fundamental role in understanding the behavior of particles at the tiny scales of atoms and subatomic particles. One of the key concepts in quantum mechanics is the notion of operators, which are mathematical objects that represent physical observables in the theory. In particular, the notion of a Hermitian operator, which corresponds to observable quantities in the physical world, is crucial to the theory. However, not all operators are Hermitian, and non-Hermitian operators can also play a role in quantum mechanics.量子力学在理解原子和亚原子粒子微观尺度行为方面起着基础性作用。
量子力学的一个关键概念是算符的概念,算符是代表理论中物理可观测量的数学对象。
特别是,埃尔米特算符的概念,它对应着物理世界中的可观测量,对于理论起着至关重要的作用。
然而,并非所有算符都是埃尔米特的,非埃尔米特算符也可以在量子力学中发挥作用。
In quantum mechanics, the observables are represented by Hermitian operators, which are essential for the statistical interpretation of the theory. Hermitian operators have realeigenvalues, which correspond to the possible measurement outcomes of physical quantities. However, non-Hermitian operators can also be used to describe certain physical systems, especially those involving open quantum systems or interactions with the environment. Although non-Hermitian operators do not correspond to observables in the same way as Hermitian operators, they can still provide important insights into the behavior of quantum systems.在量子力学中,可观测量由埃尔米特算符表示,这对于理论的统计解释至关重要。
量子相变中的量子纠缠度量研究-英文版

RG flow
• c-theorem:
cUV cIR
fixed point
(Zamolodchikov, 1986)
UV
fixed point
IR
• Massive theory (off critical) Block entropy saturation
fixed point
RG flow
UV
Irreversibility of RG trajectories
Loss of entanglement
Open Systems & Quantum Information Milano, 10 Marzo 2006
• Local Entropy: when the subsystem A is a single site.
• The concurrence measures the entanglement between two sites after having traced out the remaining sites. • The transition is signaled by the first derivative of the concurrence, which diverges logarithmically (specific heat).
h 1 lnh 1
S1 has the same singularity as
Local (single site) entropy: 1 ρ1 = I + σ z σ z S1 = Tr ρ1lnρ1 2
σz
Local measures of entanglement based on the 2-site density matrix depend on 2-point functions
开放系统理论OpenSystemsTheory

开放系统理论(Open Systems Theory)我们必须建立一个新的世界,一个更加美好的世界——在那里,人类永恒的尊严得到尊重。
——哈里〃斯科特〃杜鲁门开放系统理论的起源系统一词,来源于古希腊语,是由部分构成整体的意思。
今天人们从各种角度上研究系统,对系统下的定义不下几十种。
如说“系统是诸元素及其顺常行为的给定集合”,“系统是有组织的和被组织化的全体”,“系统是有联系的物质和过程的集合”,“系统是许多要素保持有机的秩序,向同一目的行动的东西”,等等。
我们通常把系统定义为:由若干要素以一定结构形式联结构成的具有某种功能的有机整体。
在这个定义中包括了系统、要素、结构、功能四个概念,表明了要素与要素、要素与系统、系统与环境三方面的关系。
系统思想源远流长,但作为一门科学的系统论,人们公认是美籍奥地利人、理论生物学家L.V.贝塔朗菲(L.Von.Bertalanffy)创立的。
他在1932年提出“开放系统理论”,提出了系统论的思想。
开放系统理论认为,组织是由多个部分组成的复杂系统,要把组织当作一个整体进行研究。
组织对周围环境是开放的,采取行动时为了使组织处于一个稳定的状态。
基本目标是确保生存,途径是通过改变输入和适应发生的变化。
由于组成部分包括人,所以管理者要关注工作中的人性。
贝塔朗菲认为,除了生物学方面的一些差别,人类与其他生物的区别在于符号的创造与应用,符号是人们自由创造出来的,代表某些含义,在传统中得以传播。
是思想和价值观在意识层面的反映。
贝塔朗菲的系统思考看到的是不同的符号系统或者符号领域。
他认为正是通过这种概念,语言,科学,艺术和其他文化领域,才能超越其创造者的个体和人生得以生存。
开放系统的概念指与外界环境存在物质、能量、信息交换的系统。
开放系统是一般系统论中最重要的基本概念。
开放系统的特点是系统与外界环境之间有物质、能量或信息的交换。
封闭系统则与此相反,它与外界环境之间不存在物质、能量或信息的交换。
Quantum Mechanics
Quantum MechanicsQuantum mechanics is a branch of physics that deals with the behavior of matter and energy at the atomic and subatomic level. It is a fundamental theory that has revolutionized our understanding of the physical world. However, it is also a complex and counterintuitive theory that challenges our common sense notions of reality. In this essay, we will explore the key concepts and implications of quantum mechanics from multiple perspectives.From a historical perspective, quantum mechanics emerged in the early 20th century as a response to the failure of classical physics to explain certain phenomena, such as the behavior of electrons in atoms and the blackbody radiation. The pioneers of quantum mechanics, such as Max Planck, Albert Einstein, and Niels Bohr, developed a new framework based on the idea that energy is quantized, meaning that it can only exist in discrete amounts or packets called quanta. This led to the development of the wave-particle duality, which states that particles can behave like waves and vice versa.From a theoretical perspective, quantum mechanics is based on a set of mathematical equations that describe the behavior of particles and their interactions. The most famous equation is the Schr?dinger equation, which describes the evolution of a wave function that represents the probability of finding a particle in a certain state. The wave function is a complex functionthat contains all the information about the particle's position, momentum, and other properties. However, the interpretation of the wave function is a matter of debate and controversy.From a philosophical perspective, quantum mechanics raises profound questions about the nature of reality, causality, and determinism. One of the most famous thought experiments in quantum mechanics is the Schr?dinger's cat paradox, which illustrates the concept of superposition and entanglement. In this experiment, a cat is placed in a box with a radioactive source that has a 50% chance of decaying and releasing a poison that kills the cat. According to quantum mechanics, until the box is opened and observed, the cat is in a superposition of being both alive and dead, and the act of observation collapses the wave function and determinesthe cat's fate. This raises the question of whether reality is determined by observation or whether there is an objective reality independent of observation.From a practical perspective, quantum mechanics has led to many technological innovations, such as the development of transistors, lasers, and quantum computers. The principles of quantum mechanics have also been applied to fields such as chemistry, biology, and materials science, leading to new discoveries and insights. However, the practical applications of quantum mechanics are still in their infancy, and many challenges remain, such as the problem of decoherence and the difficulty of scaling up quantum systems.From a cultural perspective, quantum mechanics has had a profound impact onour worldview and cultural imagination. It has inspired artists, writers, and filmmakers to explore the themes of uncertainty, indeterminacy, and the limits of human knowledge. It has also challenged our traditional notions of causality and determinism, leading to new forms of spirituality and mysticism. However, the cultural impact of quantum mechanics is not always positive, as it can also leadto misunderstandings and pseudoscientific beliefs.In conclusion, quantum mechanics is a fascinating and complex theory that has profound implications for our understanding of the physical world, as well as our philosophical, practical, and cultural perspectives. While it is a challenging theory that defies our common sense notions of reality, it is also a theory that has led to many technological innovations and scientific discoveries. As we continue to explore the mysteries of the quantum world, we must remain open-minded and humble in the face of its complexities and uncertainties.。
2023年全球排名前10的量子计算公司
2023年全球排名前10的量子计算公司汇总量子是一种全新的计算方式,它将对我们的世界产生巨大的影响。
让我们来了解一下量子领域的10 家领先公司量子计算具有强大的潜力和发展前景,被麦肯锡公司视为科技领域的下一个重要趋势之一,同时有预测显示,到2035 年,量子计算的价值将超过 1.3 万亿美元。
里杰蒂Rigetti Computer用超导量子位做了一些很酷的东西,它们可以让组织用量子处理器来提升自己的计算能力。
Rigetti 专门为金融、保险、制药、国防和能源领域的客户提供一些针对模拟、优化和机器学习应用的定制软件和全套解决方案。
东芝的量子密钥分发(QKD) 计划是用量子物理学的神秘定律来保护网络通信免受黑客攻击。
自从2003 年在剑桥开始搞量子密码学以来,该公司就一直在创造历史,比如2004 年第一个在100 公里光纤上传送量子密钥,还有2017 年第一个让密钥速率超过10Mbit/s。
源讯量子Atos 是数字化转型领域的大佬,目前在网络安全、云和高性能计算领域都是欧洲第一。
该公司的目标是帮助设计未来的信息空间,从而为科学和技术的进步做出贡献,同时还要尽可能地保护环境。
Atos量子学习机(QLM) 是一个超强的专用硬件设备,可以让研究人员、工程师和学生玩转量子软件。
阿里巴巴集团是中国最大的电商平台,也是全球最大的云服务提供商之一。
该公司的目标是到2036年服务全球20亿消费者,使1000万家企业实现盈利,并创造1亿个就业岗位。
2018年,它和阿里云以及中科院合作搞了一个11量子比特量子开源项目模拟器驱动的开发工具。
它可以用来做一些很牛逼的事情,比如精确模拟量子电路和收缩张量网络。
英特尔是芯片界的老大哥,它已经在搞量子计算六年了。
它的Horse Ridge II低温量子控制芯片可以让更多的量子位更紧密地集成在一起,而冷冻探测器可以让大批量测试变得更容易,这些都有助于加快商业化进程。
2023 年2 月,英特尔发布了一个软件平台,可以让开发人员构建一些很酷的量子算法,这些算法将来可以在英特尔正在努力打造的量子计算机上运行。
《2024年量子计算系统软件研究综述》范文
《量子计算系统软件研究综述》篇一一、引言随着信息技术的飞速发展,传统计算机的运算能力已经逐渐接近其物理极限。
为了突破这一极限,科学家们开始探索新的计算方式,其中最具潜力和挑战性的就是量子计算。
量子计算以其独特的并行性和指数级增长的计算能力,在信息安全、药物研发、材料设计等多个领域具有广泛应用前景。
因此,量子计算系统软件的研究与开发已成为当前计算机科学领域的重要研究方向。
本文旨在综述量子计算系统软件的研究现状、主要成果及未来发展趋势。
二、量子计算系统软件研究概述1. 量子计算系统软件的基本原理与架构量子计算系统软件是建立在量子力学原理和量子算法基础上的软件系统。
其基本原理是利用量子比特(qubit)的叠加和纠缠等特性进行信息处理。
与传统的二进制计算机相比,量子计算机可以同时处理多个信息单元,从而在处理大规模问题时展现出更高的效率和精确度。
在架构上,量子计算系统软件主要包括底层硬件接口、算法库和高级编程语言等部分。
其中,底层硬件接口用于连接量子计算机硬件设备;算法库包含了一系列可复用的量子算法模块;高级编程语言则是用于开发复杂算法的编程语言工具。
2. 量子计算系统软件的主要研究领域目前,量子计算系统软件的研究领域主要包括算法研究、编程语言与编译器设计、系统架构优化等。
其中,算法研究是量子计算的核心部分,旨在探索新的量子算法和优化现有算法;编程语言与编译器设计则是为了方便用户开发和使用量子算法;系统架构优化则是为了提高量子计算机的运算速度和稳定性。
三、国内外研究现状及主要成果1. 国内研究现状及主要成果国内在量子计算系统软件领域的研究起步较早,并在算法研究、编程语言与编译器设计等方面取得了一系列重要成果。
例如,在算法研究方面,国内学者成功设计了一系列针对特定问题的量子算法,如Shor大数分解算法、Grover搜索算法等;在编程语言与编译器设计方面,国内已经开发出多种用于开发量子算法的编程语言和编译器工具,如基于量子语言的集成开发环境等。
Mellanox Quantum 硬件和软件产品说明书
Mellanox Technologies Mellanox Quantum™ Firmware Release NotesRev 27.2000.21822Mellanox Technologies Mellanox Technologies350 Oakmead Parkway Suite 100Sunnyvale, CA 94085U.S.A. Tel: (408) 970-3400Fax: (408) 970-3403© Copyright 2019. Mellanox Technologies Ltd. All Rights Reserved.Mellanox®, Mellanox logo, Mellanox Open Ethernet®, LinkX®, Mellanox Spectrum®, Mellanox Virtual Modular Switch®, MetroDX®, MetroX®, MLNX-OS®, ONE SWITCH. A WORLD OF OPTIONS®, Open Ethernet logo, Spectrum logo, Switch-IB®, SwitchX®, UFM®, and Virtual Protocol Interconnect® are registered trademarks of Mellanox Technologies, Ltd.For the complete and most updated list of Mellanox trademarks, visit /page/trademarks.All other trademarks are property of their respective owners.NOTE:THIS HARDWARE, SOFTWARE OR TEST SUITE PRODUCT (“PRODUCT(S)”) AND ITS RELATED DOCUMENTATION ARE PROVIDED BY MELLANOX TECHNOLOGIES “AS-IS” WITH ALL FAULTS OF ANY KIND AND SOLELY FOR THE PURPOSE OF AIDING THE CUSTOMER IN TESTING APPLICATIONS THAT USE THE PRODUCTS IN DESIGNATED SOLUTIONS. THE CUSTOMER'S MANUFACTURING TEST ENVIRONMENT HAS NOT MET THE STANDARDS SET BY MELLANOX TECHNOLOGIES TO FULLY QUALIFY THE PRODUCT(S) AND/OR THE SYSTEM USING IT. THEREFORE, MELLANOX TECHNOLOGIES CANNOT AND DOES NOT GUARANTEE OR WARRANT THAT THE PRODUCTS WILL OPERATE WITH THE HIGHEST QUALITY. ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY, FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT ARE DISCLAIMED. IN NO EVENT SHALL MELLANOX BE LIABLE TO CUSTOMER OR ANY THIRD PARTIES FOR ANY DIRECT, INDIRECT, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES OF ANY KIND (INCLUDING, BUT NOT LIMITED TO, PAYMENT FOR PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY FROM THE USE OF THE PRODUCT(S) AND RELATED DOCUMENTATION EVEN IF ADVISED OF THE POSSIBILITY OF SUCHDAMAGE.Rev 27.2000.21823Mellanox Technologies Table of ContentsDocument Update History . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4Chapter 1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51.1 Supported Switch Systems. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51.2 Firmware Interoperability . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51.3 Supported Cables . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61.3.1 Validated and Supported FDR Cables . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61.3.2 Validated and Supported EDR Cables . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61.3.3 Validated and Supported HDR Cables. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61.3.4Supported Link Speed. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 71.4 Firmware Upgrade . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 71.5 PRM Revision Compatibility. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8Chapter 2 Changes and New Features. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9Chapter 3 Known Issues . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10Chapter 4 Bug Fixes History . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 12Chapter 5 Firmware Changes and New Features History. . . . . . . . . . . . . . . . 14Rev 27.2000.21824Mellanox Technologies Document Update HistoryTable 1 - Release Update HistoryRevision Date DescriptionRev 27.2000.2182October 13, 2019Initial release of this firmware version. This versionintroduces Bug Fixes (see Section 4, “Bug Fixes History,” on page 12)IntroductionRev 27.2000.21825Mellanox Technologies 1IntroductionThese are the release notes for the Mellanox Quantum™ firmware, Rev 27.2000.2182. This firm-ware complements the Mellanox Quantum™ switch with a set of advanced features, allowing easy and remote management of the switch.This firmware supports the following protocols:•InfiniBand - SDR,QDR, FDR EDR,HDR1.1Supported Switch SystemsThis firmware supports the devices listed in Table 2. For the most updated list of switches sup-ported, visit the Firmware Download pages on . 1.2Firmware InteroperabilityThis firmware version has been validated to work against platforms with the following firmware and software versions.Table 2 - Supported Switch SystemsModel Number DescriptionMQM8790Mellanox Quantum ™ 40-port Non-blocking Externally Managed HDR 200Gb/s InfiniBand Smart SwitchTable 3 - Firmware InteroperabilityHCA/SwitchFirmware Version Quantum 27.2000.2182Switch-IB 11.2000.2046Switch-IB 215.2000.2046ConnectX®-620.26.1040ConnectX®-5 Ex 16.26.1040ConnectX®-516.26.1040ConnectX®-412.26.1040ConnectX®-3 Pro 2.42.5000ConnectX®-3 2.42.5000Connect-IB®10.16.1200MFT4.13.0Note: The minimal required ConnectX-6 firmware version is 20.25.1532.Rev 27.2000.21826Mellanox Technologies 1.3Supported Cables1.3.1Validated and Supported FDR Cables1.3.2Validated and Supported EDR Cables1.3.3Validated and Supported HDR CablesTable 4 - Validated and Supported FDR CablesSpeedCable OPN #DescriptionFDR MC2207310-003Mellanox® Active Fiber Cable, VPI, up to 56Gb/s, QSFP, 3m FDR MC2207310-010Mellanox® Active Fiber Cable, VPI, up to 56Gb/s, QSFP, 10m FDR MC2207310-015Mellanox® Active Fiber Cable, VPI, up to 56Gb/s, QSFP, 15m FDRMC2207310-100Mellanox® Active Fiber Cable, VPI, up to 56Gb/s, QSFP, 100mTable 5 - Validated and Supported EDR CablesSpeed Cable OPN #DescriptionEDR MCP1600-E001Mellanox Passive Copper Cable VPI 100GB/S QSFP LSZH 1M EDR MCP1600-E002Mellanox Passive Copper Cable VPI 100GB/S QSFP LSZH 2M EDR MCP1600-E00A Mellanox Passive Copper Cable VPI 100GB/S QSFP LSZH 0.5M EDR MFA1A00-E010Mellanox Active Fiber Cable, VPI, up to 100Gb/s, QSFP, 10m EDR MFA1A00-E015Mellanox Active Fiber Cable, VPI, up to 100Gb/s, QSFP, 15m EDR MFA1A00-E100Mellanox Active Fiber Cable, VPI, up to 100Gb/s, QSFP, 100m EDRMCP1OPT-E002Mellanox® Passive Copper cable, VPI, up to 100Gb/s, QSFP, LSZH, 2mNote: EDR links raise with RS_FEC.Table 6 - Validated and Supported HDR CablesSpeed OPN # / Name DescriptionHDR MCP1650-H001E30Mellanox® Passive Copper cable, IB HDR, up to 200Gb/s, QSFP28, PVC, 1m, white pultab, 30AWGHDR MCP1650-H002E26Mellanox Passive Copper Cable, IB HDR, up to 200GB/S, QSFP56, LSZH, 2M, black pultab, 26AWGHDR MCP1650-H00AE30Mellanox Passive Copper Cable, IB HDR, up to 200GB/S, QSFP56, LSZH, 0.5M, black pultab, 30AWGHDR MCP7H50-H001R30Mellanox® Passive Copper hybrid cable, IB HDR 200Gb/s to 2x100Gb/s, QSFP56 to 2xQSFP56, LSZH, colored pulltabs, 1m, 30AWGHDRMFS1S00-H003EMellanox® active fiber cable, IB HDR, up to 200Gb/s, QSFP56, LSZH, black pulltab, 3mIntroductionRev 27.2000.21827Mellanox Technologies 1.3.4Supported Link SpeedThe table below lists the current supported link speed.1.4Firmware UpgradeFirmware upgrade may be performed directly from any previous version to this version. To upgrade firmware, please refer to the Mellanox Firmware Tools (MFT) package at:/page/management_toolsHDR MFS1S00-H005E Mellanox® active fiber cable, IB HDR, up to 200Gb/s, QSFP56, LSZH, black pulltab, 5mHDR MFS1S00-H010E Mellanox® active fiber cable, IB HDR, up to 200Gb/s, QSFP56, LSZH, black pulltab, 10mHDR MFS1S00-H100E Mellanox® active fiber cable, IB HDR, up to 200Gb/s, QSFP56, LSZH, black pulltab, 100mHDR MFS1S50-H0xxE Mellanox® active fiber splitter cable, IB HDR, 200Gb/s to 2x100Gb/s, QSFP56 to 2xQSFP56 , LSZH, up to 30mHDRMFS1S90-H003EMellanox® active fiber splitter cable, IB HDR, 2x200Gb/s to 2x200Gb/s, 2xQSFP56 to 2xQSFP56, LSZH, 3mNote: HDR links raise with RS_FEC.Table 7 - Supported Link SpeedSpeed CableCable Length LimitationsSDR Optical Up to 100MCopper Up to 2M QDROptical3/10/15/100MNote: QDR speed is only supported when using FDR cables. See Table 4,“Validated and Supported FDR Cables,” on page 6.FDR Optical 3/10/15/100M EDR Optical Up to 100M Copper Up to 3M HDROpticalUp to 100MNote: HDR optical cables support only HDR speed.Thus, when mask is configured to HDR, the link is not raised when connecting to EDR devices.Copper Up to 2MTable 6 - Validated and Supported HDR CablesSpeed OPN # / Name DescriptionRev 27.2000.21828Mellanox Technologies 1.5PRM Revision CompatibilityFirmware Rev 27.2000.2182 complies with the Mellanox Switches Programmer’s Reference Manual (PRM), Rev 1.40 or later.Changes and New FeaturesRev 27.2000.21829Mellanox Technologies 2Changes and New FeaturesTable 8 - Changes and New FeaturesCategoryDescriptionRelease 27.2000.2182GeneralBug Fixes (see Section 4, “Bug Fixes History,” on page 12)Rev 27.2000.218210Mellanox Technologies 3Known IssuesThe following sections describe known issues in this firmware release and possible workarounds.Table 9 - Known IssuesInternal Ref.Issue1886809Description: FDR speed in Quantum-base switches is supported only when using optical cables 10m\15m\30m and only on ports: #7, #9 - #30.Workaround: N/AKeywords: Cables, ports, speed1713747Description: When using splitter HDR optical cables, toggling the upper port causes the lower port to be toggled as well. Workaround: N/AKeywords: Cables, port toggling1856717Description: High BER may occur when connecting cables of type 0.5/1m DAC to an HDR speed.Workaround: N/A Keywords: Cables1761271Description: CWDM4 AOM cable is currently not supported on Quantum switch systems. Workaround: N/A Keywords: Modules/Cables1563590Description: LR4 modules are currently not supported. Workaround: N/A Keywords: Modules/Cables-Description: The supported length of HDR copper cables is currently up to 2M.Workaround: N/A Keywords: HDR cablesDescription: Although the effective BER (after FEC) is expected to meet our design targets (e.g. 10e-14 or lower), occasionally it may be higher.Workaround: N/A Keywords: Cables-Description: HDR optical cables and Split cables support only HDR speed.Workaround: N/AKeywords: Link Speed, cables, Break-Out cables-Description: The following features are currently not supported on Mellanox Quantum™ based systems:•IB Router•Congestion ControlV oltage reading via MVCR Workaround: N/AKeywords: Mellanox Quantum-Description: When using Mellanox AOC cables longer than 50m use one VL to achieve full wire speed.Workaround: N/A Keywords: CablesKnown IssuesTable 9 - Known IssuesInternal Ref.Issue955641Description: VL_HIGH_LIMIT is not affecting the VL arbiter as expected.Workaround: Arbitration table should be set using only the low priority VL arbitration table.Keywords: VL Arbitration1249608Description: Configuring weight "0" for VL, results in unexpected behavior.Workaround: Arbitration table should be configured with weights other than "0".Keywords: VL Arbitration-Description: Module info page in Diagnostics Data VS-MAD is not supportedWorkaround: N/AKeywords: Diagnostics Data VS-MAD4Bug Fixes HistoryTable 10 lists the bugs fixed in this release.Table 10 - Bug Fixes HistoryInternal Ref.Issues1899441Description: Fixed an issue that caused the packets to be transmitted from a wrong output port due to awrong configuration of the packet classification decision in the switch forwarding database cache key, thatcaused both AR eligible packets and AR ineligible packets to hit the same cache entry.Keywords:Switch forwarding, Adaptive RoutingDiscovered in Version: 27.2000.2046Fixed in Release: 27.2000.21821885460Description: On rare occasions, and under high SHARP load, switch SHARP operation might get stuck.Keywords: SHARPDiscovered in Version: 27.2000.2046Fixed in Release: 27.2000.21821859715Description: The bandwidth on MFS1S00-H050E cables is 99G/s and on MFS1S00-H100E cables is67Gb/s when connecting at HDR speed to an HDR switch.Keywords: CablesDiscovered in Version: 27.2000.1886Fixed in Release: 27.2000.20461797452Description: A port may hang while Link-Maintenance runs on it and the second port’s link istoggled.Keywords: Link-Maintenance, port togglingDiscovered in Version: 27.2000.1600Fixed in Release: 27.2000.18861698990Description: HDR link up time when using optical cables may take 6 minutes or more (up to 20minutes).Keywords: HDR, optical cables, link up timesDiscovered in Version: 27.2000.1100Fixed in Release: 27.2000.18861718734/ 1723236/ 1718645/ 1710631Description: On rare occasions, HDR link may not raise properly when using optical cables. Keywords: HDR linkDiscovered in Version: 27.2000.1012Fixed in Release: 27.2000.16001774870Description: Link flapping and packet loss during High/Low temperature changes.Keywords: LinkDiscovered in Version: 27.2000.1400Fixed in Release: 27.2000.16001778837Description: When using a copper splitter cable up to 2m length in HDR100 mode, traffic may drop.Keywords: Cable, HDR100Discovered in Version: 27.2000.1400Fixed in Release: 27.2000.1600Bug Fixes HistoryTable 10 - Bug Fixes HistoryInternal Ref.Issues1534459Description: When working with 8 VLs, TP does not function due to buffers’ configuration.Keywords: VLs, latency, performanceDiscovered in Version: 27.2000.1100Fixed in Release: 27.2000.14001605587Description: Fixed an issue that cause the green port LED to blink in the same frequency regardless of the link speed rate set.Keywords: Port LEDDiscovered in Version: 27.1910.0618Fixed in Release: 27.2000.11421598550Description: Fixed an issue that prevented the port from being split when the request (command) was sent from the NV config tool.Keywords: Split PortDiscovered in Version: 27.1910.0618Fixed in Release: 27.1910.06205Firmware Changes and New Features History Table 11 - Firmware Changes and New Features HistoryCategory DescriptionRelease 27.2000.2046Mellanox Scalable Hierarchical Aggregation and Reduction Protocol (SHARP)™[Beta] Mellanox Scalable Hierarchical Aggregation and Reduction Protocol (SHARP)™ technology improves the performance of MPI operations by offloading collective operations from the CPU to the switch network, and by eliminating the need to send data multiple times between endpoints.Link Speed Added QDR/FDR support in Quantum switch systems when using optical cables ofup to 30m.Note: QDR speed is only supported when using the FDR cables. See Table 4,“Validated and Supported FDR Cables,” on page 6Cables Removed PLR from active cables longer than 30m.Release 27.2000.1886Physical Layer Retransmission (PLR) Added support to the Physical Layer Retransmission (PLR) functionality for HDR speed.Link Speed Link-up time improvements. The link up time is up to 60 secRelease 27.2000.1600General Bug Fixes (see Section 4, “Bug Fixes History,” on page 12)Release 27.2000.1400Link Speed HDR speed rate is at GA level.Cables Added support for Break-Out Cable auto-sensing.Release 27.2000.1142Link Speed HDR link stability enhancements.Note: HDR is at beta level.Release 27.2000.1012Link Speed HDR speed rate is currently at Beta level.Release 27.2000.1004Link Speed Stability improvements for HDR link.Subnet Manager (Adaptive Routing)Added support for Adaptive Routing. Adaptive routing (AR) allows optimizing data traffic flow. The InfiniBand protocol uses multiple paths between any two points. Thus, when unexpected traffic patterns cause some paths to be overloaded, AR can automatically move traffic to less congested paths according to the current temporal state of the network.Adaptive Routing Added support for Private Linear Forwarding Tables (PLFT). This capability helpsSM to optimize traffic.Release 27.1930.0016Link speed Added support for EDR rate speed.Note: For MLNX-OS software version (3.7.1074) to properly work, you must useQuantum unmanaged firmware v27.1930.0016 and above, and ConnectX-6firmware v20.99.6044 and above.Firmware Changes and New Features HistoryTable 11 - Firmware Changes and New Features HistoryCategory DescriptionRelease 27.1930.0012Cables Added support for Copper cables up to 2m at HDR speed.Added support for Optic cables up to 100m at HDR speed.Added support for break-out cables for both copper and optics, at HDR speed.Release 27.1920.0016Link Speed HDR link rise time optimizations.Release 27.1920.0012Power Consumption Improved Quantum switch based system’ power consumption.Release 27.1920.0008Link Speed[Alpha Quality] Added support for HDR speed when using optical cables toconnect between switches (switch to switch connection).Release 27.1920.000Link Speed[Alpha Quality] Added support for 3 & 10 meter optical cables when in loopbackmode at HDR link speed on the front end (edge) ports only.[Alpha Quality] Added support for 1 & 15 meter HDR copper cables whenconnected to a ConnectX-6 adapter cards at EDR link speed.Release 27.1910.0Bug Fixes See Section 4, “Bug Fixes History,” on page 12Release 27.1910.0618General This is the initial GA firmware version for Mellanox Quantum™ 40-port Non-blocking Externally Managed HDR 200Gb/s InfiniBand Smart Switch(MQM8790).Note: This firmware version supports SDR and EDR speeds only.Split Port Enables the user to split a single physical quad-lane QSFP port into 2 dual-laneports using the break-out cable.。
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Minisymposium15OperatortheorieLeiter des Symposiums:Prof.Dr.Birgit Jacob Dr.Carsten TrunkTechnical University Delft Technische Universit¨at BerlinFac.EWI/TWAP.O.Box5031Straße des17.Juni1362600GA Delft,The Netherlands10623Berlin,GermanyDie Operatortheorie besch¨aftigt sich mit der Analyse linearer Abbildungen auf unend-lichdimensionalen R¨aumen.Einen besonderen Schwerpunkt bildet dabei die Spektral-theorie,die Erweiterungstheorie symmetrischer Operatoren,die Fredholmtheorie und die Theorie der Halbgruppen.148Minisymposium15Montag,18.SeptemberHS IV,Hauptgeb¨aude,Regina-Pacis-Weg14:30–15:20Klaus-Jochen Engel(University of L’Aquila,Italy) Boundary control offlows in networks15:30–15:50Andras B´atkai(ELTE TTK/Institute of Mathematics) Differenzialgleichungen mit Verz¨ogerung in L p Phasenr¨aumen16:00–16:20Peer Kunstmann(Karlsruhe)L q-Eigenschaften elliptischer Randwertprobleme16:30–16:50Markus Biegert(Ulm)Elliptic Problems on Varying DomainsDienstag,19.SeptemberH¨orsaal411AVZ I,Endenicher Allee11-1315:00–15:50Christiane Tretter(Bremen)Spectral problems for block operator matrices in hydrodynamics16:00–16:20Matthias Langer(University of Strathclyde,Glasgow) Variational principles for eigenvalues of the Klein–Gordon equation16:30–16:50Monika Winklmeier(Bremen)Estimates for the eigenvalues of the angular part of the Dirac equation in the Kerr-Newman metric17:00–17:20Annemarie Luger(TU Berlin)On a result for differential operators with singular potentials17:30–17:50Jussi Behrndt(University of Groningen)Open Quantum SystemsOperatortheorie149 Mittwoch,20.SeptemberH¨orsaal411AVZ I,Endenicher Allee11-1315:00–15:50Hagen Neidhardt(WIAS Berlin)Perturbation theory of semi-groups and evolution equations16:00–16:20Bernhard Haak(TU Delft)A stochastic Datko-Pazy theorem16:30–16:50Tanja Eisner(T¨ubingen)Fast schwache Konvergenz von Operatorhalbgruppen17:00–17:20Carsten Trunk(TU Berlin)Location of the spectrum of operator matrices which are associated to second order equations17:30–17:50Birgit Jacob(TU Delft)A resolvent test for admissibility of Volterra observation operators150Minisymposium15Vortragsausz¨ugeKlaus-Jochen Engel(University of L’Aquila,Italy)Boundary control offlows in networksWe investigate a boundary control problem on a network.We study a transport equation in the network,controlling it in a single vertex.We describe all the possible reachable states and prove a criterium of Kalman type for the vertices in which the problem is controllable.This is joint work with Marjeta Kramar Fijav(Ljubljana),Rainer Nagel(T¨ubingen)and Eszter Sikolya(Budapest).Andras B´atkai(ELTE TTK/Institute of Mathematics) Differenzialgleichungen mit Verz¨ogerung in L p Phasenr¨aumenIm Vortrag wird ein halbgruppentheoretischer Zugang zu Differenzialgleichungen mit Verz¨ogerung in L p Phasenr¨aumen pr¨asentiert.Dies erm¨oglicht uns die Verz¨ogerung in eine additive St¨orung zu verwandeln und erm¨oglicht dadurch die Anwendung der reichen St¨orungstheorie der Halbgruppen.Neben diesem Zugang werden auch die Er-gebnisse neuester spektraltheoretischer Untersuchungen gezeigt.Referenzen:B´atkai,A.,Piazzera,S.,“Semigroups for Delay Equations in L p-Phase Spaces”,Rese-arch Notes in Mathematics vol.10,A.K.Peters:Wellesley MA,2005.B´atkai,A.,Eisner,T.,Latushkin,Y.,The spectral mapping property of delay semigroups, submittedPeer Kunstmann(Karlsruhe)L q-Eigenschaften elliptischer RandwertproblemeWir untersuchen L q-Eigenschaften elliptischer Randwertproblemeλu−Au=f inΩ⊂R nBu=g auf∂Ω.Operatortheorie151 Hierbei ist im einfachsten Fall A= jk a jk∂j∂k ein Differentialoperator mit a jk∈L∞, B= j b j∂j ein Differentialoperator erster Ordnung mit b j∈C0,1,sowie f∈L q(Ω)und g∈W1,q(Ω).Ausgehend von Absch¨atzungen wie|λ| u q+ ∇2u q≤C( f q+|λ|1/2 g q+ ∇g q)f¨ur ein festes q∈(1,∞)und hinreichend großeλin einem geeigneten Sektor zei-gen wir verallgemeinerte Gauß-Absch¨atzungen und mit deren Hilfe weitere Eigenschaf-ten wie R-Sektorialit¨at,R-Beschr¨anktheit der L¨osungsoperatoren und maximale L p-L q-Regularit¨at f¨ur die induzierte analytische Halbgruppe.Markus Biegert(Ulm)Elliptic Problems on Varying DomainsThe aim of this talk is to show optimal results on local and global uniform convergence of solutions to elliptic equations with Dirichlet boundary conditions on varying domains. We assume that the limit domain be stable in the sense of Keldyˇs.We further assume that the approaching domains satisfy a necessary condition in the inside of the limit domain,and only require L2-convergence outside.As a consequence,uniform and L2-convergence are the same in the trivial case of homogenisation of a perforated domain.Christiane Tretter(Bremen)Spectral problems for block operator matrices in hydrodynamicsIn the linear stability analysis of hydrodynamics,the spectra of non-symmetric systems of coupled differential equations have to be studied.As examples,we consider the Ekman boundary layer problem and the Hagen Poiseuilleflow with non-axisymmetric disturbances.In both cases we investigate the essential spectrum by means of operator theoretic methods.(joint work with M.Marletta,Cardiff)152Minisymposium15Matthias Langer(University of Strathclyde,Glasgow)Variational principles for eigenvalues of the Klein–Gordon equationWe consider eigenvalues of the Klein–Gordon equation,which can be written as a quadratic eigenvalue problem.Under certain assumptions the continuous spectrum has a gap and we can characterise eigenvalues in this gap even in the presence of complex eigenvalues.This quadratic eigenvalue problem can also be linearised in a Pontryagin space.Connections between the negative index of the Pontryagin space and the index shift in the variational principle are presented.Monika Winklmeier(Bremen)Estimates for the eigenvalues of the angular part of the Dirac equation in theKerr-Newman metricThe radial part of the Dirac equation describing a fermion in the Kerr-Newman back-ground metric has an operator theoretical realisation as a block operator matrix A= −D B B∗D with domain D(A)=D(B∗)⊕D(B)in the Hilbert space H=L2(0,π)2.It can be shown that the spectrum of A consists of eigenvalues only.We will show that the expression A−λallows for a factorisation into three factors such that all the information about the spectrum of A is contained in a scalar operator valued function.From this function we obtain a lower bound for the smallest eigenvalue in modulus of A.Another method to obtain such a bound is to use techniques related to the quadratic nuermical range of block operator matrices.Annemarie Luger(TU Berlin)On a result for differential operators with singular potentialsWe explore the connection between a(generalized)Titchmarsh-Weyl-coefficient for the singular Sturm-Liouville operator(y):=−y (x)+ q0x2+q1x y(x)on x∈(0,∞),with q0>3and q1∈R,and a certain singular perturbation of this operator.This talk is based on joint work with Pavel Kurasov(Lund).Operatortheorie153 Jussi Behrndt(University of Groningen)Open Quantum SystemsOpen quantum systems are often described with a maximal dissipative operator A D, a so-called pseudo-Hamiltonian,and a self-adjoint operator A0in some Hilbert space H.If L denotes a minimal self-adjoint dilation of A D,i.e.,L acts in a Hilbert space H⊕L2(R,K)such that P H(L−λ)−1|H=(A D−λ)−1,and L0=A0⊕−i d dx,then thescattering matrix of the closed system{L,L0}can be recovered from the scattering matrix of the dissipative system{A D,A0}.Since in this model L is not semibounded from below serious doubts arise from a physical point of view.We propose a slightly different approach where instead of afixed pseudo-Hamiltonian A D a family of energy dependent pseudo-Hamiltonians{A−τ(λ)}is considered.The outer space L2(R,K)is replaced by some Hilbert space K and the Hamiltonian L in H⊕K satisfies P(L−λ)−1|H=(A−τ(λ)−λ)−1and is often semibounded from below. We show that the scattering matrix of the closed system can be recovered in a similar way as above and that the model with onefixed pseudo-Hamiltonian can be regarded as an approximation.The abstract theory is illustrated with some examples.The talk is based on joint work with Mark M.Malamud(Donetsk National University, Ukraine)and Hagen Neidhardt(WIAS,Berlin).Hagen Neidhardt(WIAS Berlin)Perturbation theory of semi-groups and evolutionequationsThe aim of the present talk is to develop an approach to the Cauchy problem for linear evolution equations of type∂u(t)+A(t)u(t)=0,u(s)=u s,a<s≤t<b,∂ton a separable Banach space X,where(a,b)is afinite open interval and{A(t)}t∈(a,b)is a family of closed linear operators on the separable Banach space X.The main questi-on concerning the Cauchy problem is tofind a so-called“solution operator”or propaga-tor U(t,s).We are going to solve this problem embedding it into a perturbation problem for generators of semi-groups in the Banach space L p([0,T],X),1<p<∞.The ab-stract existence results are applied to Schr¨odinger operators with time-dependent point interactions.154Minisymposium15Bernhard Haak(TU Delft)A stochastic Datko-Pazy theoremThe well-known Datko-Pazy theorem states that if(T(t))t≥0is a strongly continuous semigroup on a Banach space E such that all orbits T(·)x belong to the space L p(R+,E) for some p∈[1,∞),then(T(t))t≥0is uniformly exponentially stable,or equivalently, there exists an >0such that all orbits t→e t T(t)x belong to L p(R+,E).We show that a similar result also hold for so-calledγ–radonifying operators,namely the equivalence of1.For all x∈E,T(·)x∈γ(R+,E).2.There exists an >0such that for all x∈E,t→e t T(t)x∈γ(R+,E).If E is a Hilbert space,γ(R+,E)=L2(R+,E)and we reobtain Datko’s theorem mentio-ned above.γ–radonifying operators play an important role in the study abstract stocha-stic Cauchy problems on E whence the result can also be seen as a perturbation result for stochastic Cauchy problems.References:B.Haak,M.Veraar,J.van Neerven:A stochastic Datko-Pazy theorem,submitted; avaiable on ArXiv.Tanja Eisner(T¨ubingen)Fast schwache Konvergenz von OperatorhalbgruppenF¨ur C0-Halbruppen auf Banachr¨aumen diskutieren wir den Zusammenhang zwischen Spektraleigenschaften des Generators und der Konvergenz der Halbgruppe f¨ur t→∞(insbesondere f¨ur die schwache Topologie).Carsten Trunk(TU Berlin)Location of the spectrum of operator matrices which are associated to second order equationsWe study second order equations of the form¨z(t)+A o z(t)+D˙z(t)=0.Operatortheorie155 Here the stiffness operator A o is a possibly unbounded positive operator on a Hilbert space H,which is assumed to be boundedly invertible,and D,the damping operator,is an unbounded operator,such that A−1/2o DA−1/2o is a bounded non negative operatoron H.This second order equation is equivalent to the standardfirst-order equation ˙x(t)=Ax(t),where A:D(A)⊂D(A1/2o)×H→D(A1/2o)×H,is given byA= 0I−A o−D ,D(A)= [z w]∈D(A1/2o)×D(A1/2o)|A o z+Dw∈H .This block operator matrix has been studied in the literature for more than20years.It is well-known that A generates a C0-semigroup of contraction,and thus the spectrum of A is located in the closed left half plane.We are interested in a more detailed study of the location of the spectrum of A in the left half plane.In general the(essential)spectrum of A can be quite arbitrary in the closed left half plane.Under various conditions on the damping operator D we describe the location of the spectrum and the essential spectrum of A.The talk is based on joint work with Birgit Jacob(Delft).Birgit Jacob(TU Delft)A resolvent test for admissibility of Volterra observation operatorsNecessary and sufficient conditions are given forfinite-time admissibility of a linear sy-stem defined by a Volterra integral equation when the underlying semigroup is equiva-lent to a contraction semigroup.These necessray and sufficient conditions are in terms of a pointwise bound on the resolvent of the infinitesimal generator.This generalizes an analogous result known to hold for the standard Cauchy problem.The talk is based on joint work with Jonathan R.Partington(University of Leeds).。