数字集成电路面试常见问题
Space exploration was always fascinating, and recent developments have reignited the interest to the heights never seen since the last man stood on the Moon. People argue about Mars exploration and features of spaceships as their grandparents would’ve done if the internet existed fifty years ago. I’m an electronics engineer working in the aerospace industry, so I know a thing or two about the technical background of this stuff — and I see that these things aren’t common knowledge, and people often have significantly skewed ideas about the reasons behind some devices and decisions. Namely, I’d love to speak about some misconceptions related to radiation hardened integrated circuits and the means of their protection against radiation-induced damage. But, I warn you, this text will be relatively long.
太空探索总是令人着迷,最近的发展使人们对自最后一个人站在月球上以来从未见过的高度重新产生了兴趣。 人们争论着火星的探索和宇宙飞船的特征,就像互联网在五十年前存在时他们的祖父母所做的那样。 我是航空航天业的电子工程师,所以我对这些技术的背景知识了解一两件事,而且我发现这些知识不是常识,人们通常对背后的原因有明显的偏见一些设备和决定。 即,我很想谈谈与辐射硬化集成电路有关的一些误解,以及防止辐射引起的损害的保护手段。 但是,我警告您,这段文字会比较长。
The most popular theses about radiation hardness of ICs are the following:
关于IC辐射硬度的最受欢迎的论文如下:
Radiation hardened chips are not needed at all. CubeSats are just fine with chips from the nearest store, very ordinary Lenovo laptops work on the ISS without any problems, and even NASA-commissioned Orion onboard computer is based on a commercial microprocessor!
根本不需要经过辐射硬化的芯片。 CubeSats可以与附近商店的芯片配合使用,非常普通的Lenovo笔记本电脑可以在ISS上正常工作,甚至NASA委托的Orion车载计算机都基于商用微处理器!
Satellites don’t need computational power, but they need these magical radiation hardened chips, so most of them use very old but extremely robust designs from the eighties, like TTL quad NAND gates.
卫星不需要计算能力,但是它们需要这些神奇的辐射硬化芯片,因此大多数卫星都使用80年代的非常古老但极其坚固的设计,例如TTL四与非门。
A thesis that complements the previous one: it is impossible to achieve radiation hardness on modern process nodes. Ionizing particles just tear small transistors apart. So, the use of these TTL NAND gates is not just justified, it’s the only way to go.
这是对前一个论文的补充:在现代Craft.io节点上不可能达到辐射硬度。 电离粒子只会将小的晶体管撕开。 因此,使用这些TTL NAND门并不合理,这是唯一的方法。
It’s necessary and sufficient to use silicon on insulator (SOI) or silicon on sapphire (SOS) technology to achieve radiation hardness.
必须使用绝缘体上硅(SOI)或蓝宝石上硅(SOS)技术来达到辐射硬度。
All military-grade chips are radiation hardened and all radiation hardened chips are military-grade. If you have a military-grade IC, you can safely launch it into outer space.
所有军用级芯片都经过辐射硬化,所有防辐射芯片都经过了军工级认证。 如果您拥有军用级IC,则可以安全地将其发射到太空中。
As one can see, these theses directly contradict each other — which makes arguing on the internet even funnier, especially if you take into account that not a single one of them is true.
可以看到,这些论点直接相互矛盾,这使在互联网上争论变得更加有趣,尤其是如果考虑到其中没有一个是真的。
Let’s start with an important disclaimer: radiation hardness is not the Holy Grail of integrated design for space and other similar environments. It’s just a bunch of checkboxes in the long requirements list, which typically includes reliability, longevity, wide temperature range, tolerance to electrostatic discharge, vibrations and many more. Everything that can compromise reliable functioning through the entire lifetime is important, and most applications requiring radiation tolerance also assume the impossibility of repair or replacement. On the other hand, if something is wrong with one of the parameters, system-level designers of the final can often find a workaround — tighten temperature requirements, use cold spares or additional protection circuitry — whatever is suitable. The same approach can be fine when dealing with radiation effects: majority voting, supply current control and reset are very common means that are often effective. But it's also often when a brand new radiation hardened IC is the only good way to meet mission requirements.
让我们从一个重要的免责声明开始:辐射硬度不是用于太空和其他类似环境的集成设计的圣杯。 在很长的要求列表中,它只是一堆复选框,通常包括可靠性,寿命,宽温度范围,对静电放电的耐受性,振动等等。 在整个生命周期内都会影响可靠功能的所有因素都很重要,并且大多数需要防辐射的应用也都认为不可能进行修理或更换。 另一方面,如果其中一个参数出了点问题,则最终的系统级设计人员通常可以找到解决方法-严格控制温度,使用冷备件或附加保护电路-适用。 处理辐射效应时,可以使用相同的方法:多数表决,电源电流控制和重置是非常有效的非常普遍的方法。 但是,通常只有全新的辐射硬化IC是满足任务要求的唯一好方法。
It is also useful to remember that the developers of special-purpose systems are the same people as any other developers. Just like anyone else, they normally write code filled with crutches to be ready for yesterday's deadline and want more powerful hardware to mask their sloppy job; some would’ve used Arduino if it was properly certified. And it’s also obvious that people who create requirements are rarely really concerned with any limitations and want to have the same as in commercial systems, but more reliable and radhard. Therefore, modern processes are more than welcome in radhard electronics — system designers would love to have large amounts of DRAM, multi-core processors, and the most advanced FPGAs. I have already mentioned that there could be workarounds for mediocre radiation tolerance, so the use of commercial chips is mostly limited by the lack of data on what problems are than by the problems themselves or by the commercial status of the chips.
记住,专用系统的开发人员与任何其他开发人员都是同一个人,这也很有用。 就像其他任何人一样,他们通常会写满拐杖的代码,以准备在昨天的截止日期前完成工作,并希望有更强大的硬件来掩盖他们的草率工作。 如果经过适当的认证,有些人会使用Arduino。 同样显而易见的是,创建需求的人很少真正关心任何限制,并希望与商业系统中的局限性相同,但更可靠,更可靠。 因此,现代Craft.io在radhard电子产品中非常受欢迎-系统设计人员希望拥有大量DRAM,多核处理器和最先进的FPGA。 我已经提到过,对于中等的辐射耐受性可能存在变通办法,因此商用芯片的使用主要受到缺乏关于什么问题的数据的限制,而不是受到问题本身或芯片商业地位的限制。
The very concepts of "radiation hardness" and "radiation hardened IC" are enormous simplifications. There are many different sources of ionizing and non-ionizing radiation, and they affect the functioning of microelectronic devices in multiple ways. The tolerance to different sets of conditions and varying levels of exposure for different applications is not the same, so a “radiation hardened” circuit designed for low earth orbit is absolutely not obliged to work in a robot parsing debris in Chernobyl or Fukushima.
“辐射硬度”和“辐射硬化IC”这两个概念非常简化。 电离辐射和非电离辐射有许多不同的来源,它们以多种方式影响微电子设备的功能。 对于不同的条件,对于不同的条件集和不同的暴露水平,其容忍度是不一样的,因此,绝对不需要在切尔诺贝利或福岛的机器人中使用为低地球轨道设计的“辐射硬化”电路来解析碎片。
Ionizing radiation is called so because the deceleration of an incoming particle in a substance releases the energy and ionizes the substance. Each material has its own energy required for ionization and the creation of an electron-hole pair. For silicon it is 3.6 eV, for its oxide — 17 eV, for gallium arsenide — 4.8 eV. The energy release can also “shift” an atom out of the correct place in the crystal lattice (21 eV must be transferred to shift a silicon atom). Electron-hole pairs created in a substance can produce different effects in an integrated circuit. Therefore, radiation effects can be divided into the four large groups: the effects of total ionizing dose (TID), the dose rate effects, single event effects (SEE), and the non-ionizing effects called the displacement damage. This separation is somewhat arbitrary: for example, irradiation with a stream of heavy ions causes both single event effects and accumulation of a total ionizing dose.
之所以称为电离辐射,是因为物质中传入粒子的减速会释放能量并使物质离子化。 每种材料都有其自身的能量,这些能量用于电离和创建电子-空穴对。 硅为3.6 eV,氧化物为17 eV,砷化镓为4.8 eV。 能量释放还可以使原子“移出”晶格中的正确位置(必须转移21 eV才能移出硅原子)。 在物质中产生的电子-空穴对可以在集成电路中产生不同的效果。 因此,辐射效应可分为四大类:总电离剂量(TID)效应,剂量率效应,单事件效应(SEE)和称为位移损伤的非电离效应。 这种分离在某种程度上是任意的:例如,重离子流的照射会导致单事件效应和总电离剂量的累积。
The total absorbed dose of radiation is measured in units called “rad”, with an indication of the substance absorbing the radiation. 1 rad = 0.01 J/kg, it’s the amount of energy released in an elementary unit of weight in a given substance. Gray, which is a 100 rad (or 1 J/kg) is another, albeit, rarer unit. It is somewhat important to understand the same amount of ionizing particles released by a source of radiation (called radiation exposure) will be translated into different levels of absorbed dose in different substances. The material of choice for silicon ICs is silicon oxide. That’s because very low hole mobility in SiO2 causes charge accumulation in oxide producing various total dose effects. Typical dose levels for commercial circuits are in the range of 5-100 krad (SiO2). The levels that are in actual demand for some practical applications start around 30 krad (SiO2) and go as far as a few Grad (SiO2), depending on the purpose of the chip. Yes, Gigarads. The lethal dose for a human is around 6 Gray.
辐射的总吸收剂量以称为“ rad”的单位进行测量,并指示吸收辐射的物质。 1 rad = 0.01 J / kg,它是指定物质中基本重量单位释放的能量。 灰色是100弧度(或1焦耳/千克),是另一个虽然较稀有的单位。 了解辐射源释放的相同数量的电离颗粒(称为辐射暴露)将转化为不同物质中不同剂量的吸收剂量,这一点有点重要。 硅IC的选择材料是氧化硅。 这是因为SiO2中非常低的空穴迁移率会导致氧化物中的电荷积累,从而产生各种总剂量效应。 商业电路的典型剂量水平在5-100 krad(SiO2)的范围内。 在某些实际应用中,实际需要的电平大约为30 krad(SiO2),最高可达几个Grad(SiO2),具体取决于芯片的用途。 是的,吉加拉德。 一个人的致死剂量约为6格雷。
The TID effects are mostly associated with the accumulation of positive charge in dielectrics. They manifest themselves in CMOS circuits in several main ways:
TID效应主要与电介质中正电荷的积累有关。 它们以几种主要方式出现在CMOS电路中:
Threshold voltage shift. For n-channel transistors, the threshold is usually reduced (but the dependence may be non-monotonic, especially at high doses), while for p-channel transistors it increases. The shift magnitude correlates to gate oxide thickness and decreases with process node. In older technologies, n-MOSFET threshold shift can cause functional failure when n-channel transistors stop closing and p-channel ones stop opening. This effect is less important in submicron technologies, but it can still give a lot of headaches to analogue designers.
阈值电压漂移。 对于n沟道晶体管,阈值通常会降低(但相关性可能是非单调的,尤其是在高剂量时),而对于p沟道晶体管,阈值会增加。 偏移量与栅极氧化物的厚度相关,并且随Craft.io节点而减小。 在较旧的技术中,当n沟道晶体管停止关闭而p沟道晶体管停止打开时,n-MOSFET阈值偏移会导致功能故障。 在亚微米技术中,这种影响并不那么重要,但是它仍然会使模拟设计人员感到头疼。
Leakage currents flow through parasitic channels opened by an excessive charge in isolating oxides, either from source to drain of the same device, or from one transistor to another. In the first case, a parasitic transistor controlled by the total dose is formed in parallel to the main one. The severity of this effect is highly technology-dependent as the exact shape of isolated oxide matters. Therefore, there is no direct correlation to process nodes, and there is no good way to guess which commercial device will have better or worse TID hardness.
漏电流流过由隔离氧化物中的过量电荷打开的寄生通道,这些寄生通道从同一器件的源极到漏极,或者从一个晶体管流向另一个晶体管。 在第一种情况下,由总剂量控制的寄生晶体管与主晶体管并联形成。 这种影响的严重程度在很大程度上取决于技术,因为隔离氧化物的确切形状至关重要。 因此,与Craft.io节点没有直接关系,也没有很好的方法来猜测哪个商业设备的TID硬度会更好或更差。
Charge carrier mobility decreases due to scattering on accumulated defects. The influence of this factor on submicron digital circuits on silicon is small, but it is a way more important for power transistors (including GaN HEMT).
电荷载流子迁移率由于累积缺陷上的散射而降低。 这个因素对硅上的亚微米数字电路的影响很小,但是对于功率晶体管(包括GaN HEMT)而言,这是一种更为重要的方法。
1/f noise increase caused by parasitic edge transistors. It is important for analogue and radio frequency circuits and becomes more important at lower process nodes when the influence of other TID effects gradually decreases.
由寄生边缘晶体管引起的1 / f噪声增加。 这对于模拟和射频电路很重要,并且在其他TID效应的影响逐渐减小时,在较低的过程节点处变得尤为重要。
A quick word on bipolars: the main TID effect there is gain decrease due to leakage-related base current increase. Another bipolar-specific effect is their (non-mandatory) rough reaction to the dose collection at low speed, so-called ELDRS (Enhanced Low Dose Rate Sensitivity). This effect complicates the testing and makes it more expensive. And the worst part is that many CMOS circuits contain a few bipolars (namely in voltage reference circuits) — and therefore can also be susceptible.
一个关于双极的简短说明:由于泄漏相关的基极电流增加,主要的TID效应会导致增益降低。 另一个双极特异性效应是它们在低速下对剂量收集的(非强制性)粗略React,即所谓的ELDRS(增强的低剂量率敏感性)。 这种效果使测试复杂化并使其更加昂贵。 最糟糕的是,许多CMOS电路都包含一些双极性(即在参考电压电路中),因此也容易受到影响。
Another effect related to dose rate is when dose accumulation is so fast that such a large number of electron-hole pairs is generated that a huge excessive electric charge is overflowing every node in the chip and is causing a temporary loss of functionality and sometimes a latchup of parasitic thyristor between supply and ground. The non-functioning time is the usual measure of sensitivity to this kind of effect and it's normally seen in military standards like Mil-Std-883.
与剂量率有关的另一个影响是,剂量累积如此之快,以至于产生了如此大量的电子-空穴对,以至于芯片中的每个节点都溢出了巨大的过量电荷,并导致功能暂时性丧失,有时甚至闭锁电源和地之间的寄生晶闸管的数量。 非工作时间是对这种影响的敏感度的通常度量,通常在军事标准(如Mil-Std-883)中看到。
Total dose rate effects are the reason for “silicon on sapphire” (SOS) and “silicon on insulator” (SOI) technology creation and adoption: the best way to reduce the amount of charge inserted into active devices by the flow of ionizing particles is to cut their electrical connection to the enormously big substrate (and to each other). Why are these effects important? An extremely high dose rate for a short time is a typical consequence of a nuclear explosion, and military guys all around the world deeply care about this matter. Luckily for us, SOI proved to be advantageous in many other applications and therefore became widespread in normal life.
总剂量率效应是创建和采用“蓝宝石上的硅”(SOS)和“绝缘体上的硅”(SOI)技术的原因:减少通过电离粒子流插入有源器件中的电荷量的最佳方法是切断它们与非常大的基板(以及彼此之间)的电连接。 为什么这些影响很重要? 短时间内的极高剂量率是核爆炸的典型结果,世界各地的军方对此事都深表关切。 对我们来说幸运的是,SOI在许多其他应用中被证明是有优势的,因此在正常生活中变得越来越普遍。
Single event effects (SEE) are associated with a measurable effect from the strike of a single ionizing particle. They can be divided into two large groups:
单事件效应(SEE)与单个电离粒子撞击的可测量效应相关。 它们可以分为两大类:
Non-destructive events include bit flips or upsets (SEU) in a variety of storage elements (cache memory cells, register files, FPGA configuration memory, etc.) and transient voltage spikes (SET) in combinational logic and in analogue circuits. The main feature of these effects is that they do not lead to the physical destruction of the chip and can be corrected by software or hardware. Moreover, single event transients are self-corrected after some arbitrarily short time. Memory upsets are the most known of these effects as they constitute a lion's share of failures due to the enormous amount of memory in modern digital ICs.
无损事件包括各种存储元件(高速缓存存储单元,寄存器文件,FPGA配置存储器等)中的位翻转或翻转(SEU),以及组合逻辑和模拟电路中的瞬态电压尖峰(SET)。 这些影响的主要特征是它们不会导致芯片的物理损坏,可以通过软件或硬件进行纠正。 此外,单事件瞬变会在任意短时间后自动校正。 存储器故障是这些影响中最著名的,因为现代数字IC中存在大量的存储器,因此它们构成了故障的绝大部分。
Destructive events are Single-Event latchup (SEL) effect and a variety of fortunately rarer catastrophic failures like transistor burnout of gate rupture. Their distinctive feature is that they are, well, destructive and irreversibly damage the chip if occurred. The specific case of the latchup is distinctive as the very fast power off can often (but not always!) save the chip. Circuits for supply current monitoring and cycling are fairly popular as a latchup protection measure. Other destructive effects uncommon on CMOS circuitry, but are a serious threat for some types of flash memory and for high voltage devices, including power switches.
破坏性事件包括单事件闩锁(SEL)效应以及各种幸运的罕见灾难性故障,例如晶体管对栅极破裂的烧坏。 它们的独特之处在于,它们一旦发生就会具有破坏性且不可逆转地损坏芯片。 闩锁的特殊情况很独特,因为非常快速的断电通常可以(但不总是如此)节省芯片。 作为闭锁保护措施,用于电源电流监视和循环的电路相当流行。 其他破坏性影响在CMOS电路上并不常见,但对某些类型的闪存和包括电源开关在内的高压设备则构成严重威胁。
Figure 1. Experimental data on single event effects rate. Taken from J. Barth et al., "Single event effects on commercial SRAMs and power MOSFETs: final results of the CRUX flight experiment on APEX", NSREC Radiation Effects Data Workshop, 1998
图1.单事件影响率的实验数据。 摘自J. Barth等人,“对商用SRAM和功率MOSFET的单事件效应:在APEX上进行CRUX飞行实验的最终结果”,NSREC辐射效应数据研讨会,1998年
Looking at figure 1, one can see that the worst case is about one upset per two hundred days... per bit. Yes, every bit in memory is about to be affected twice per years. But when we have Megabits or Gigabytes of memory, it's always compromised, right? Yes, that's a problem, and there are techniques to address this problem, but more on that a bit later.
从图1可以看出,最坏的情况是每200天……每位发生一次故障。 是的,内存中的每一位每年将受到两次影响。 但是,当我们拥有兆位或千兆字节的内存时,它总是会受到损害,对吧? 是的,这是一个问题,并且有一些技术可以解决此问题,但稍后会对此进行更多介绍。
The specific energy yield of an ionizing particle strike is called “linear energy transfer” (LET) and is measured (MeV * cm^2)/mg. LET non-linearly and non-monotonously depends on particle energy and is also related to the path length, which can vary from hundreds of nanometers to hundreds of millimeters for relevant particles and materials. Basically, most ionizing particles just punch through an IC and fly back to outer space. Low energy particles are much more common in a real space environment (see Figure 2). Important LET values are 30 (corresponding to ions of iron) and 60/80 (which are normally considered the highest LET values to be taken into account). Another important figure is 15 MeV * cm ^ 2/(mg) — the maximum LET of products of the nuclear reaction between a silicon atom and a proton or a neutron. Protons are important as they make up a significant part of solar radiation. Whilst they have very low LET on their own, the probability of the above mentioned nuclear reaction is high enough to create a lot of events, especially in van Allen belts or during solar bursts. Protons can also interact with nuclei of heavier elements, like tungsten (used in contacts) or tantalum (popular anti-TID shielding material). Such secondary effects are the second most important reason not to pack your space-bound chips into led covers in an attempt to increase their radiation hardness. The first one is, by the way, the launch price per kilo.
电离粒子撞击的比能量产率称为“线性能量转移”(LET),并以(MeV * cm ^ 2)/ mg进行测量。 LET非线性且非单调取决于粒子能量,并且还与路径长度有关,对于相关的粒子和材料,路径长度可能从数百纳米到数百毫米不等。 基本上,大多数电离粒子只是穿过IC,然后飞回太空。 在现实空间环境中,低能粒子更为常见(请参见图2)。 重要的LET值是30(对应于铁离子)和60/80(通常被认为是要考虑的最高LET值)。 另一个重要的数字是15 MeV * cm ^ 2 /(mg)-硅原子与质子或中子之间的核React产物的最大LET。 质子很重要,因为它们构成了太阳辐射的重要组成部分。 尽管它们自己的LET很小,但上述核React的可能性很高,足以引发很多事件,尤其是在范艾伦带或太阳爆发时。 质子还可以与重元素的原子核相互作用,例如钨(用于接触)或钽(常用的抗TID屏蔽材料)。 这种次要效果是第二个最重要的原因,不要将空间受限的芯片包装到LED盖中,以提高其辐射硬度。 顺便说一下,第一个是每公斤的价格。
It’s also worth noting helium nuclei (alpha particles) as a source of single event effects — not because there are some in solar radiation, but because plenty of alpha sources can be found in ordinary life, like led solder and some IC packaging materials. If you have heard about low-alpha bumps and underfills — it’s about single event mitigation in “mundane” applications not related to aerospace.
还值得一提的是,氦原子核(α粒子)是单事件效应的来源-并不是因为太阳辐射中有一些,而是因为在日常生活中会发现大量的α辐射源,例如led焊料和某些IC封装材料。 如果您听说过低阿尔法的颠簸和底部填充,那就是与航空航天无关的“平凡”应用中的单事件缓解。
Figure 2. A number of different particles spotted during the two-year mission in space. Quoted from: Xapsos et al., "Model for Cumulative Solar Heavy Ion Energy and Linear Energy Transfer Spectra", IEEE Transactions on Nuclear Science, Vol. 5, No. 6., 2007
图2.在为期两年的太空任务中发现的许多不同粒子。 引自:Xapsos等人,“累积太阳重离子能量和线性能量转移谱的模型”,IEEE Transactions on Nuclear Science,第1卷。 5,第6号,2007年
1, 30 or 60 MeV * cm ^ 2/(mg) — how much is it? The upset threshold of a standard SRAM memory cell in the 7 nm technology is much lower than one, while for 180 nm it can vary from one to ten. The use of a special schematic allows to raise the threshold up to a hundred, but it is usually wiser to achieve 15 or 30 and to the rest via error-correcting codes. 60 MeV * cm ^ 2/(mg) can most often be found in requirements for destructive events — to ensure that the chip will highly likely survive its full intended lifespan.
1、30或60 MeV * cm ^ 2 /(mg)-多少? 7纳米技术中的标准SRAM存储单元的翻转阈值远低于1,而180纳米的阈值则可以从1改变为10。 使用特殊的原理图可以将阈值提高到一百,但是通常更明智的做法是通过纠错码将阈值提高到15或30,然后达到其余值。 60 MeV * cm ^ 2 /(mg)最经常出现在破坏性事件的要求中-以确保芯片极有可能在其预期的整个使用寿命中幸存下来。
The displacement effects are local destruction of the crystal lattice due to an atom being "knocked out" of its intended place. The energy required for this is usually quite high, so most irradiating particles do not cause this effect. However, secondary irradiation can, and there are plenty of protons in space. These local lattice defects decrease charge carriers’ mobility, increase noise and do some other damage. Due to their very local nature, they normally do not significantly affect conventional CMOS chips — but they dominate in solar cells, photodetectors, power transistors and other devices based on compound semiconductors, such as gallium arsenide and gallium nitride. Transistors in compound semiconductors are usually not MOS, but JFET or HEMT, so they lack gate oxide. This explains their high total dose tolerance — they simply do not suffer from the effects causing the rapid degradation of CMOS chips. However, displacement effects are much more significant in these new materials, so they should be considered and weighted appropriately.
位移效应是由于原子“敲除”其预期位置而导致的晶格局部破坏。 为此所需的能量通常很高,因此大多数辐射粒子不会引起这种效果。 但是,可以进行二次辐照,并且空间中有很多质子。 这些局部晶格缺陷会降低电荷载流子的迁移率,增加噪声并造成其他一些损害。 由于它们的局部特性,它们通常不会显着影响传统的CMOS芯片-但它们在太阳能电池,光电探测器,功率晶体管和其他基于化合物半导体的器件(例如砷化镓和氮化镓)中占主导地位。 复合半导体中的晶体管通常不是MOS,而是JFET或HEMT,因此它们缺少栅极氧化物。 这解释了它们的高总剂量耐受性-它们根本不会遭受导致CMOS芯片快速退化的影响。 但是,位移效应在这些新材料中更为重要,因此应考虑并适当权衡它们。
As we’re finished with the description of effects, let’s look at where and how they threaten integrated circuits.
完成对效果的描述后,让我们看一下它们在哪里以及如何威胁集成电路。
Figure 3. Total ionizing dose calculations, for ten years of satellite lifetime, under the shielding of 1 g/cm^2. Adapted from N. Kuznetsov, "Radiation danger on space orbits and interplanetary trajectories of satellites" (in Russian).
图3.在1 g / cm ^ 2的屏蔽下,十年卫星寿命的总电离剂量计算。 改编自库兹涅佐夫(N. Kuznetsov),“卫星的空间轨道和行星际轨道上的辐射危险”( 俄语 )。
Figure 3 shows an example of total ionizing dose calculation for different orbits. There are multiple assumptions there — including solar activity, shape, material and thickness of protection, but you can get the idea: the dose rate can vary in five orders of magnitude at different orbits. At low orbits under the first Van Allen belt, the dose is absorbed so slowly that many out-of-the-shelf commercial chips can withstand several years in these conditions, like laptops at ISS do. Even much more fragile people can fly there for years without dramatic health consequences. Low orbits are extremely important as they encompass the entire manned astronautic, the Earth remote sensing, many present communication satellites and future internet-from-above constellations. Last but not least, almost all CubeSats are launched into low orbits.
图3显示了不同轨道总电离剂量计算的示例。 那里有多种假设-包括太阳活动,形状,材料和保护层的厚度,但是您可以理解:剂量率在不同的轨道上可以变化五个数量级。 在第一个Van Allen带下的低轨道上,剂量吸收得如此缓慢,以至于许多现成的商用芯片在这种情况下都可以承受数年,就像ISS的笔记本电脑一样。 甚至更脆弱的人也可以在那飞行很多年而不会造成严重的健康后果。 低轨道非常重要,因为它们涵盖了整个载人航天,地球遥感,许多现有的通信卫星以及未来的互联网之上的星座。 最后但并非最不重要的一点是,几乎所有的CubeSat卫星都被送入低轨道。
Actually, the importance of low orbits is the root of multiple speculations that expensive radiation hardened chips are not needed at all, and COTS can do everything if not rejected by the overly conservative industry. Yes, COTS can do some decent job, but there are some pitfalls, even at low orbits.
实际上,低轨道的重要性是多种猜测的根源,即根本不需要昂贵的辐射硬化芯片,而且如果过度保守的行业不拒绝,COTS可以做所有事情。 是的,COTS可以做一些体面的工作,但是即使在低轨道上也有一些陷阱。
The van Allen belts protect the Earth only from light particles, mainly solar electrons and protons. Heavier particles, even though they are much rarer, quietly reach even our last shield — the atmosphere — and cause single effects, including the catastrophic latchup capable of irreversibly destroying any chip at any moment. Therefore, commercial chips can be used only if they are somehow protected from the latchup, or the entire spacecraft can be lost.
范艾伦带仅保护地球免受轻粒子(主要是太阳电子和质子)的侵害。 较重的粒子,即使它们稀少得多,也可以悄悄地到达我们的最后一道盾牌-大气-并产生单一的影响,包括灾难性的闩锁,该闩锁能够在任何时候不可逆转地破坏任何芯片。 因此,只有在某种程度上保护了商业芯片免受闩锁,否则整个航天器可能会丢失,才可以使用它们。
Another problem is that the chips used in space are not just processors and memory, but also many other types, including power and analogue ones. Radiation tolerance of non-logic circuits is much more complex, less investigated and less predictable. Moreover, modern SoCs contain a lot of non-digital blocks like PLL, ADC, I/O circuits. For example, the most common reason for flash memory total dose failure is the high-voltage generator used for memory writing. Analogue circuits suffer from offset increase, small leakages can significantly affect the functioning of low-power analogue, power transistors are experiencing breakdown voltage degradation, and so on and so on.
另一个问题是,空间中使用的芯片不仅是处理器和内存,而且还有许多其他类型,包括电源和模拟类型。 非逻辑电路的辐射容忍度要复杂得多,研究较少且难以预测。 此外,现代SoC包含许多非数字模块,例如PLL,ADC,I / O电路。 例如,闪存总剂量失败的最常见原因是用于存储器写入的高压发生器。 模拟电路的失调增加,小泄漏会严重影响低功率模拟电路的功能,功率晶体管正遭受击穿电压降级等。
It’s also important to remember that radiation sensitivity is, well, sensitive to process variations, sometimes even small ones. So, if the fab changes the temperature of some oxide growing, you can throw your radiation testing results into a trash can. Commercial vendors never guarantee that the different batches of the same product will have the same crystal and that the manufacturing process will be stable for some long time. The processor from iPhone 6, Apple A9, was produced on both 16 nm TSMC and 14 nm Samsung fabs, and the user is ineligible to know which version is inside the specific cell phone. Such an approach is unfortunately impossible for high-reliability circuits, and that’s why radhard chips are often manufactured on some kinds of Trusted Foundries or at least on automotive-intended processes, as the car industry also cares about reliability and needs stable technology.
同样重要的是要记住,辐射敏感性对Craft.io变化敏感,有时甚至很小。 因此,如果制造厂改变了某些氧化物生长的温度,则可以将辐射测试结果扔到垃圾桶中。 商业供应商永远不能保证同一产品的不同批次具有相同的晶体,并且制造过程将长期稳定。 iPhone 6,Apple A9的处理器是在16 nm TSMC和14 nm Samsung fab上生产的,用户无资格知道特定手机内的哪个版本。 不幸的是,这种方法对于高可靠性电路是不可能的,这就是为什么radhard芯片通常在某些类型的Trusted Foundry或至少在汽车预期的Craft.io上制造的原因,因为汽车行业还关心可靠性并需要稳定的技术。
However, satellites don’t fly just on low orbits. I will take a “Molniya” orbit as an example of very different requirements. This orbit is named after a Soviet satellite which was there first. “There” is a polar orbit with minimal altitude around 500 km and maximal around 40 000. The orbital period is twelve or twenty-four hour, and the satellite spends most of the time near apogee, acting as a pseudo-static object and providing communications for polar regions where geostationary satellites can’t be seen.
但是,卫星不仅会在低轨道上飞行。 我将以“莫利尼亚”轨道为例说明完全不同的要求。 该轨道以最早出现的苏联卫星命名。 “那里”有一条极地轨道,其最小高度在500公里左右,最大高度在4万左右。轨道周期为十二或二十四小时,卫星大部分时间都在近地点附近,充当伪静态物体并提供无法看到对地静止卫星的极地通信。
Figure 4. Molniya orbit with hours marked. Taken from Wikipedia.
图4.标记了小时数的摩利尼亚轨道。 取自维基百科。
The lifespan of the very first Molniya satellites was very short — just a handful of months. Primarily due to the degradation of solar panels powering radio transmitters. Why was the degradation so high? Perigee 500 km and apogee 40 000 km means that the satellite crosses van Allen belts twice each period — or four times per day. Van Allen belts gather and concentrate solar electrons and protons, so the environment there is among the worst one can have.
最早的Molniya卫星的寿命很短-仅几个月。 主要是由于为无线电发射器供电的太阳能电池板的性能下降。 为什么降解如此之高? 近地点500公里和远地点40 000公里,意味着卫星每个周期两次穿过范艾伦带-每天四次。 范艾伦带聚集并聚集太阳能电子和质子,因此那里的环境是最恶劣的环境之一。
Figure 1 promises the dose rate of some tens of kilorads per ten-year lifespan on high orbits and some hundreds of thousand if the satellite is in contact with van Allen belts. That’s higher than many commercial chips can achieve, so one will need significantly thicker, heavier and more expensive shielding to use them. It may still be cheaper than buying radiation hardened ICs, but here we descend into the world of satellite creation, which is out of this article’s scope. Let’s just say that shielding is heavy and therefore expensive to launch while it doesn’t solve all problems and can even make some of them worse.
图1保证了在高轨道上每十年寿命约数十万拉德的剂量率,如果卫星与范艾伦带接触,则约数十万的剂量率。 这比许多商用芯片所能达到的要高,因此使用它们将需要明显更厚,更重且更昂贵的屏蔽层。 它可能仍然比购买防辐射的IC便宜,但在这里我们进入了人造卫星的世界,这不在本文的讨论范围之内。 我们只能说屏蔽很重,因此发射起来很昂贵,但不能解决所有问题,甚至会使其中一些问题变得更糟。
The ultimate answer to a question if COTS chips can be used in space is “Yes, but”. There are many opportunities, but also many constraints. Also, if you want to use a COTS chip in your space-related project and invest in its radiation testing, stockpile your ten-year need. By the way, it’s a credible business-model: well-known and very respected company 3DPlus tests a lot of COTS chips chooses ones that are accidentally better than others and then packs them into their own hybrid modules found everywhere in space, including Curiosity Rover on Mars.
对于是否可以在太空中使用COTS芯片的问题,最终的答案是“是,但是”。 机会很多,但约束也很多。 另外,如果您想在与太空有关的项目中使用COTS芯片并投资其辐射测试,则可以存储10年的需求。 顺便说一句,这是一种可靠的商业模式:知名且备受推崇的公司3DPlus对许多COTS芯片进行了测试,选择了偶然比其他芯片更好的芯片,然后将它们包装到太空中随处可见的自己的混合模块中,包括好奇号流浪者在火星上。
It’s impossible to avoid the topic of “military-grade” chips while dealing with preconceptions about radiation hardness. They are believed to be radiation hardened, but the real situation is a bit more complicated. Not all military-grade chips are radhard and not all radhard chips are military-grade. If we look into the US military standard Mil-Std-883, we will find there a lot of different environmental tests — for thermal cycling, humidity, air with sea salt, etc. etc.
在处理有关辐射硬度的先入之见时,不可避免地要避免使用“军用级”芯片这一话题。 它们被认为可以防辐射,但是实际情况要复杂一些。 并非所有军事级芯片都是radhard,也不是所有radhard芯片都是军事级。 如果我们查看美国军事标准Mil-Std-883,就会发现有很多不同的环境测试-用于热循环,湿度,含海盐的空气等。
Radiation is addressed in the following paragraphs:
下列段落讨论了辐射:
1017.2 Neutron irradiation
1017.2中子辐照
1019.8 Ionizing radiation (total dose) test procedure
1019.8电离辐射(总剂量)测试程序
1020.1 Dose rate induced latchup test procedure
1020.1剂量率诱导的闩锁测试程序
1021.3 Dose rate upset testing of microcircuits
1021.3微电路剂量率不合格测试
1023.3 Dose rate response of linear microcircuits
1023.3线性微电路的剂量率响应
Total dose? Check! Total dose rate? Check. Single events? Sorry, nothing to find here. Many specifications for military-grade radhard chips include the requirements for single event effects, but they are not part of the military standard. So, “military-grade” status does not guarantee that the chip will be capable to work in space, or at Large Hadron Collider. The best-known example of this misconception in action was the infamous Russian satellite called “Phobos-Grunt”. It was sent to Mars in 2011, but never left Earth’s orbit. The official investigation concluded that the fatal failure occurred in American military-grade SRAM chip which some poor engineer found to be suitable for space travel while it wasn’t in fact protected from single event latchup.
总剂量? 检查! 总剂量率? 检查一下 单项活动? 抱歉,在这里找不到任何内容。 军用级radhard芯片的许多规范都包括对单事件效果的要求,但它们不是军用标准的一部分。 因此,“军用级”状态不能保证芯片能够在太空或大型强子对撞机上工作。 这种误解在行动中最著名的例子是臭名昭著的俄罗斯卫星“ Phobos-Grunt”。 它于2011年被送往火星,但从未离开地球轨道。 官方调查得出的结论是,致命故障发生在美国军用级SRAM芯片上,一些可怜的工程师发现该芯片适合于太空旅行,而实际上却没有受到单事件闩锁的保护。
Recent SEE testing of 1M and 4M monolithic SRAMs at Brookhaven National Laboratories has shown an extreme sensitivity to single-event latchup (SEL). We have observed SEL at the minimum heavy-ion LET available at Brookhaven, 0.375 MeV-cm2/mg
Brookhaven国家实验室最近对1M和4M单片SRAM的SEE测试表明,它对单事件闩锁(SEL)具有极高的敏感性。 我们已经在布鲁克海文获得的最小重离子LET下观察到SEL,0.375 MeV-cm2 / mg
says the report on that very chip. The report was published in 2005, but wasn’t taken into account by “Phobos-Grunt” designers, who just supposed that “military-grade” is enough to fly to the Red planet.
那个芯片上的报告说。 该报告于2005年发布,但“ Phobos-Grunt”设计人员并未考虑到该报告,他们只是认为“军事级”足以飞往红色星球。
The importance of radiation hardness is not limited to space and military applications. The atmosphere works as the final shield between the space radiation and the life on Earth, but also creates secondary particles, which are aplenty at the airliner heights (a typical transatlantic flight can see a dozen of single event upsets in the onboard computer). Some secondary particles even reach the ground and are seen in the devices with the highest memory sizes — like supercomputers. X-ray radiation is routinely used in medicine, and radiotherapy is an important way to combat malignant tumours. More and more electronics are needed in medical devices, and these areas aren't an exception.
辐射硬度的重要性不仅限于太空和军事应用。 大气层是空间辐射与地球生命之间的最终屏障,但还会产生次级粒子,这些粒子在客机高度上非常丰富(典型的跨大西洋飞行可以在机载计算机上看到许多单事件扰动)。 一些次级粒子甚至到达地面,并在具有最大内存大小的设备(例如超级计算机)中看到。 X射线通常在医学中使用,放射疗法是对抗恶性肿瘤的重要方法。 医疗设备中需要越来越多的电子设备,这些领域也不例外。
And, of course, we should not forget that all the fuss with lead-free solder was partially caused by the fact that lead and some other materials used in IC fabrication contain impurities of heavy elements like uranium. The use of these materials cause the generation of a small, but still well-measurable flux of alpha particles — right around vulnerable silicon. In the case of BGA packages or 3D assemblies — over the entire surface of vulnerable silicon.
而且,当然,我们不应该忘记,无铅焊料的所有问题都部分是由于铅和IC制造中使用的某些其他材料包含重元素(如铀)的杂质造成的。 这些材料的使用会导致在易损硅周围产生少量但仍可测量的α粒子通量。 对于BGA封装或3D组件-在易损硅的整个表面上。
Luckily, alpha particles have a rather short ionization track (just a few microns, depending on energy), and multi-layer metallization helps to reduce their influence. The bad news is that at low process nodes the required energy is so small that all alpha particles, which are able to reach the surface, cause upsets. For example, TSMC published an article at the 2018 IEEE International Reliability Physics Symposium, measuring the number of alpha-related upsets in 7 nm SRAM. So, the problem still exists in a largely lead-free world.
幸运的是,α粒子具有相当短的电离轨迹(取决于能量,仅几微米),多层金属化有助于减少其影响。 坏消息是,在低Craft.io节点处,所需的能量是如此之小,以至于所有能够到达表面的α粒子都会引起不安。 例如,台积电(TSMC)在2018年IEEE国际可靠性物理研讨会上发表了一篇文章,测量了7 nm SRAM中与alpha相关的翻转次数。 因此,在很大程度上无铅的世界中仍然存在该问题。
Figure 5. Solder bumps as the alpha radiation source. Image courtesy of Mitsubishi Materials.
图5.焊料凸点作为α辐射源。 图片由三菱综合材料提供 。
I also want to say a few words on yet another application of radiation hardened chips: high energy physics and nuclear industry. Hadron colliders and nuclear power plants require extremely robust electronics capable of working in contaminated active zones for many years. The same would be the case for robots designed to deal with nuclear-related catastrophes like Chernobyl or Fukushima. TID requirements for these circumstances could be dozens or even hundreds of Megarads (Si), which is three orders of magnitude more than in conventional space applications. The problem is further complicated by the fact that such durability is required not just from digital ICs, but also from power management and analog chips, which could be found in multichannel telemetry systems and servo motor drives. These chips could be much more vulnerable than digital ICs in terms of their reaction to transistor degradation. TID behaviour and hardening of digital circuits is well-investigated and well understood, but for analog circuits, it’s much more interesting as every case and every circuit may require an individual approach rather than a semi-automated application of known methods. The electric circuit is often guarded know-how in analog design, and it’s more true for radhard analog.
我也想谈谈辐射硬化芯片的另一种应用:高能物理和核工业。 强子对撞机和核电站需要极其坚固的电子设备,这些电子设备必须能够在受污染的活动区域中工作多年。 设计用于应对切尔诺贝利核电站或福岛核电站核灾难的机器人也是如此。 在这种情况下,TID要求可能为数十甚至数百兆拉(Si),这比常规太空应用要大三个数量级。 由于不仅需要数字IC还需要这种耐用性,而且还需要电源管理和模拟芯片来提供这种耐用性,这一问题变得更加复杂,在多通道遥测系统和伺服电机驱动器中都可以找到这种耐用性。 就其对晶体管退化的React而言,这些芯片可能比数字IC更加脆弱。 TID行为和数字电路的强化已经得到了充分的调查和很好的理解,但是对于模拟电路,它更有趣,因为每种情况和每种电路都可能需要单独的方法,而不是已知方法的半自动化应用。 电路在模拟设计中通常是受保护的专有技术,对于radhard模拟而言更是如此。
Figure 6. Normal and radiation hardened bandgap voltage reference. Taken from Y. Cao et al., «A 4.5 MGy TID-Tolerant CMOS Bandgap Reference Circuit Using a Dynamic Base Leakage Compensation Technique», IEEE Transactions on Nuclear Science, Vol.60, No.4, 2013
图6.正常和辐射硬化的带隙电压基准。 摘自Y. Cao等人的《使用动态基极泄漏补偿技术的A 4.5 MGy耐TID CMOS带隙基准电路》,IEEE核科学学报,第60卷,第4期,2013年
Let's look at a good (and rare) example of such a task. Bandgap reference voltage source is a simple and well-known circuit that could be found in any analog IC. This circuit normally contains a pair of bipolar transistors controlled by an operational amplifier. These bipolars show significant leakage under irradiation, and this leakage leads to significant output voltage changes, sometimes 10-20% under high doses, which corresponds to the effective ADC resolution of two to three bits. The circuit at the right shows reference voltage variation within 1% (which gives us more than 7 bits) under the total dose of 4.5 MGy. As you may see, it wasn’t easy to achieve this outstanding result: local feedbacks are scattered everywhere, subtracting base current from the equation and therefore getting rid of leakage current too. This radhard version contains four times more transistors and has two times more power consumption than its conventional analog. The worst is that, as I’ve said, every circuit normally requires an individual approach, making analog radhard designer's work very challenging. And there’s also a single event effects problem, solution for which is as well badly formalized and very circuit-dependent.
让我们看一下此类任务的一个好例子(很少见)。 带隙基准电压源是一种简单且众所周知的电路,可以在任何模拟IC中找到。 该电路通常包含一对由运算放大器控制的双极晶体管。 这些双极型器件在辐照下显示出明显的泄漏,这种泄漏导致显着的输出电压变化,有时在高剂量下会发生10-20%的变化,这相当于2到3位的有效ADC分辨率。 右边的电路显示在4.5 MGy的总剂量下,参考电压变化在1%以内(给我们提供了超过7位)。 如您所见,要获得如此出色的结果并不容易:局部反馈分散在各处,从等式中减去基极电流,因此也消除了泄漏电流。 该radhard版本的晶体管数量是其常规模拟产品的四倍,功耗也要高出两倍。 最糟糕的是,正如我已经说过的,每个电路通常都需要一种单独的方法,这使得模拟radhard设计人员的工作非常具有挑战性。 此外,还有一个单一的事件影响问题,其解决方案形式化很差且与电路密切相关。
The website of one established microelectronics fab with old links to the aerospace industry for a long time contained a statement that radiation tolerance could not be achieved at process nodes below 600 nm, as “charged particles pierce silicon and destroy transistors”. Surprisingly, but likely unrelated, the minimal available process node for that fab, whose high-ranking official said in the interview that it’s “technologically impossible” to create radiation hardened ICs at nodes lower than 90 nm. You may guess what was the minimal node at that fab. I was quite surprised to read that interview as I was working on a radhard 65 nm chip at that moment. I can understand some marketing nonsense, but such words are dangerous in the long term, especially when said to the wide audience or to the audience of decision-making persons.
一家建立了很久的微电子制造厂的网站已经很长时间了,它与航空航天业有着很长的联系,该网站的声明中说,在“低于600 nm的Craft.io节点”上无法达到辐射耐受性,因为“带电粒子会刺穿硅并破坏晶体管”。 令人惊讶的是,但可能与之无关的是,该晶圆厂的最小可用Craft.io节点,其高级官员在接受采访时表示,“在技术上不可能”在低于90 nm的节点上制造辐射硬化IC。 您可能会猜到那个晶圆厂的最小节点是什么。 当我当时正在研究radhard 65 nm芯片时,我很惊讶地读到这篇采访。 我可以理解一些营销上的胡说八道,但是从长远来看,这样的用语很危险,尤其是对广大受众或决策者的受众而言。
I also regularly see the reasoning that ICs built on coarse process nodes are SEL-immune due to very high energy required to influence transistors, so the long-time use of proven technology is not just justified, but simply necessary. Or vice versa, sub-something process nodes work with very low supply voltages — too low to exhibit SEL as parasitic thyristor simply can’t open. Or there are opinions that the problem is not in process nodes, it’s CMOS technology that is fundamentally weak (as evidenced by some tests done by the applicant in early seventies), while in good old time radhard ICs were bipolar/SOI/GaAs. So, since CMOS technology is fundamentally flawed, there is no other way than to continue using ancient tech for spaceships. Preferably, electronic lamps.
我还经常看到这样的理由,由于影响晶体管的能量非常高,因此在粗糙的Craft.io节点上构建的IC不受SEL的影响,因此长期使用成熟的技术不是合理的,而是很必要的。 反之亦然,子级Craft.io节点可在非常低的电源电压下工作-太低而无法展示SEL,因为寄生晶闸管根本无法打开。 或者有观点认为问题不在于Craft.io节点,而在于CMOS技术从根本上是薄弱的(如申请人在七十年代初所做的一些测试所证明的),而在较早的时期,radhard IC是双极性/ SOI / GaAs。 因此,由于CMOS技术从根本上来说是有缺陷的,因此除了继续将古老的技术用于宇宙飞船之外,别无他法。 优选地,电子灯。
For the sake of justice, some old ICs built on multi-micron process nodes are really insensitive to single events. But “some” doesn’t mean “all”, and all kinds of problems were documented through the history of space exploration. Large process nodes understandably require a lot of energy from ionizing particle fo flip a bit — but they also require the same amount of energy at each switching during normal operation, so I wish a lot of luck to anyone willing to build an Intel Core processor equivalent out of 74-series logic and I would love to see a rocket that would be able to lift such a monster into the air.
为了公正起见,一些建立在微米Craft.io节点上的旧IC确实对单个事件不敏感。 但是“一些”并不意味着“全部”,并且通过太空探索的历史记录了各种问题。 可以理解,大型过程节点需要一点点电离粒子的翻转才能消耗大量能量,但是在正常运行期间,每次切换它们也需要相同量的能量,因此,我希望对愿意构建与之等效的Intel Core处理器的所有人感到好运从74系列逻辑中脱颖而出,我很想看到一枚能够将这种怪兽升空的火箭。
On the other hand, microelectronics is not limited to microprocessors and memory. There is a huge variety of tasks where latest process nodes are not necessary, unprofitable or simply unsuitable. The global market for IC built on 200 mm wafers (process node 90 nm and above) has been growing for several years, up to a periodic shortage of production equipment. “Outdated” fabs produce both old and new designs, and many manufacturing companies are commercially successful despite not being on par with TSMC and Samsung. So, take all process node fuss with a grain of salt when data processing isn’t the topic.
另一方面,微电子不限于微处理器和存储器。 有许多任务不需要最新的过程节点,无利可图或根本不合适。 基于200毫米晶圆(Craft.io节点90纳米及以上)构建的IC的全球市场已经增长了几年,直至生产设备的周期性短缺。 “过时”的晶圆厂生产新旧设计,尽管与台积电和三星不相上下,但许多制造公司在商业上都取得了成功。 因此,当数据处理不是主题时,请对所有过程节点大惊小怪。
Other factors inciting the use of older process nodes in aerospace are a longer life cycle of such products, expensive certification and small production quantities. The design of a simple 180 nm IC could cost a few million Euro, and when these millions plus few more millions required for certification and testing are divided by a thousand ICs, each of these ICs becomes very expensive. And what if we need to recoup a few hundred millions for a 7-5 nm design? These troubles lead to two things. First, the design of most radiation hardened ICs in the world is government-subsidized. Second, successful designs are manufactured as long as it’s possible, and IPs from them are reused and reused and reused to lower costs, forcing the manufacturer to stay at the proved process node. These factors combined could create an illusion that most radhard ICs are outdated. The clients also support proven projects, or, to be more precise, flight-proven projects. If a chip has a heritage in space, it’s a colossal competitive advantage, and you may be sure that this advantage is exploited as long as possible, even when the design itself becomes outdated.
促使在航空航天中使用较旧的过程节点的其他因素是此类产品的使用寿命更长,认证费用昂贵且生产量少。 一个简单的180 nm IC的设计可能要花费几百万欧元,而当数以百万计的认证和测试所需的数百万美元除以一千个IC时,这些IC中的每一个都会变得非常昂贵。 如果我们需要为7-5 nm设计赔偿几亿美元呢? 这些麻烦导致两件事。 首先,世界上大多数辐射硬化IC的设计都是由政府补贴的。 第二,成功的设计要尽可能地进行制造,而来自它们的IP可以重复使用,再利用和再利用以降低成本,从而迫使制造商留在经过验证的过程节点上。 这些因素加在一起可能会造成大多数radhard IC已过时的幻觉。 客户还支持经过验证的项目,或更准确地说,是经过飞行验证的项目。 如果芯片在太空中具有传统,那将是一项巨大的竞争优势,即使设计本身已经过时,您也可以确保尽可能多地利用这一优势。
The public image of radhard ICs is then further diminished by the fact that the most famous of them are used in long-term scientific missions. In 2015, I’ve seen a lot of news like “the New Horizons has the same CPU as 20-year-old original Sony Playstation”. Well said, well said. The New Horizons was launched in 2006, its development had begun in 2000 — it was the year of the first flight of the processor they used. Mongoose-V processor shares the MIPS ISA with PlayStation's MIPS R3000, but it’s entirely different chip released in 1998, some eight years before the launch of the New Horizons and seventeen years before it was featured in the news. Here is another example: Power750 processors came out for commercial applications in 1997, particularly for iMac computers. Their radhard counterpart, RAD750, was released in 2001 and flown into space in 2005, four years later. It was the highest computational power available for the Curiosity Mars Rover, so there was a lot of news about an ancient processor on Mars later in 2012. And, to make it even funnier, almost the entire Curiosity design was reused for the Perseverance, which is due to produce more stupid processor-related news headlines next year.
由于最著名的radhard IC用于长期科学任务,因此进一步降低了radhard IC的公众形象。 在2015年,我看到了很多新闻,例如“ New Horizons与拥有20年历史的原始Sony Playstation具有相同的CPU”。 说得好,说得好。 New Horizons于2006年推出,其开发工作于2000年开始-这是他们使用的处理器首次飞行的一年。 Mongoose-V处理器与PlayStation的MIPS R3000共享MIPS ISA,但它与1998年发布的芯片完全不同,这是在New Horizon发布之前大约8年,而在新闻发布之前已是17年。 这是另一个示例:Power750处理器于1997年投入商业应用,尤其是iMac计算机。 他们的radhard对应机RAD750于2001年发布,并于四年后于2005年飞入太空。 这是“好奇号”火星探测器所具有的最高计算能力,因此在2012年晚些时候有很多关于火星上的古老处理器的消息。而且,更有趣的是,几乎整个“好奇号”设计都被重新用于“恒心”计划,明年将产生更多与处理器相关的愚蠢新闻头条。
Despite all of the above, the newest radhard ICs of today are designed at the nodes between 45 and 20 nm, like fresh radhard Xilinx Kintex FPGAs. American RAD5500 series is manufactured at 45 nm, European DAHLIA, which is due in 2021, uses 28 nm, and so on. GlobalFoundries already offers a 12 nm process for aerospace applications, so the modern radhard ICs are definitely modern.
尽管有上述所有内容,但今天的最新radhard IC是在45至20 nm之间的节点上设计的,就像新鲜的radhard Xilinx Kintex FPGA一样。 美国RAD5500系列以45 nm制造,欧洲DAHLIA将于2021年制造,使用28 nm,依此类推。 GlobalFoundries已经为航空航天应用提供了12 nmCraft.io,因此现代radhard IC绝对是现代的。
There are many topics to be researched and there is no shortage of scientific articles on the topic of radiation hardness of modern technologies as new challenges tend to emerge with each new generation. Process node shrinking definitely affects radiation hardness, but this effect is complex and not necessarily negative. The general trend is that TID influence decreases while the role of single events becomes more important. Thinner gate oxides lead to smaller threshold voltage shifts, but then these gate oxides are not silicon oxide anymore, and their interface with silicon is different, and so on and so on.
有很多课题需要研究,关于现代技术的辐射硬度这一主题的科学文章也不乏,因为每一代人都面临着新的挑战。 Craft.io节点的收缩肯定会影响辐射硬度,但是这种影响是复杂的,不一定是负面的。 总体趋势是,TID影响减小,而单个事件的作用变得更重要。 较薄的栅极氧化物会导致较小的阈值电压漂移,但是这些栅极氧化物不再是氧化硅,它们与硅的界面也不同,依此类推。
Figure 7. Two versions of radiation hardened inverter. Taken from Vaz et al., "Design Flow Methodology for Radiation Hardened by Design CMOS Enclosed-Layout-Transistor-Based Standard-Cell Library", Journal of Electronic Testing, volume 34, 2018
图7.两种版本的防辐射逆变器。 取自Vaz等人,“通过基于设计CMOS封闭布局晶体管的标准单元库对辐射进行硬化的设计流方法论”,电子测试杂志,第34卷,2018年
Figure 7 shows two implementations of an inverter. On the right, we see a complete stuffing — enclosed layout transistors to combat total dose and individual guard rings against Inter-transistor leakages and SEL. On the right — a simpler design for lower total dose requirements: transistors are linear. It’s worth noting that total dose tolerance of 50-100 krad(Si) is quite sufficient for many space applications, and normal linear transistors do an excellent job there while saving area, not suffering from aspect ratio limitation and having better matching than ELTs. Also note that only nMOSFETs suffer from source-drain leakage and only they have to have enclosed gates if high total dose tolerance is needed, but pMOSFETs are often drawn as ELTs too for easier size balancing between nMOS and pMOS.
图7显示了逆变器的两种实现。 在右侧,我们看到了一个完整的填充物-封闭的布局晶体管以抵抗总剂量,并设有单独的保护环以防止晶体管间泄漏和SEL。 右侧-一种用于降低总剂量的更简单设计:晶体管为线性。 值得注意的是,50-100 krad(Si)的总剂量容限对于许多空间应用来说已经足够了,普通的线性晶体管在节省空间的同时也做得很好,而不会受到长宽比的限制,并且比ELT具有更好的匹配性。 还要注意的是,只有nMOSFET受源漏泄漏的困扰,如果需要高的总剂量容限,则只有封闭的栅极,但为了使nMOS和pMOS之间的尺寸平衡更加容易,pMOSFET也经常被用作ELT。
Single events’ relationship with process nodes is more interesting. Approximate diameter of the charge collection area of an ionizing particle hit is around one micron — which is much bigger than the size of memory cells in deep submicron process nodes. And indeed, experiments show multiple bit upsets from a single ion strike.
单个事件与流程节点的关系更加有趣。 电离粒子撞击的电荷收集区域的近似直径约为1微米-远大于深亚微米Craft.io节点中存储单元的大小。 实际上,实验表明,一次离子撞击会造成多个位不安。
Figure 8. Multiple bit upsets in two different 6T SRAM cell arrays. Taken from M. Gorbunov et al., "Design of 65 nm CMOS SRAM for Space Applications: A Comparative Study", IEEE Transactions on Nuclear Science, Vol.61, No.4, 2014
图8.两个不同的6T SRAM单元阵列中的多个位翻转。 取自M. Gorbunov等人,“用于太空应用的65 nm CMOS SRAM设计:比较研究”,IEEE Transactions on Nuclear Science,第61卷,第4期,2014年
Figure 8 shows the experimental data on single-event upsets in 65 nm bulk technology. On the left — normal commercial 6T-SRAM design. Ten upsets from the single hit! Hamming code won’t protect you from such disaster. So, when we’re talking about commercial ICs, coarse process nodes are somewhat better than smaller ones, as they will mostly experience easier to correct single-bit upsets. But when we’re designing a radhard chip form the scratch, there are a plethora of architectural, schematic and layout solutions capable to produce both high single event tolerance and high performance. The right side of figure 8 also shows the results from 6T-SRAM, from the same die, with the same schematic, but with a different layout. The price of getting rid of most multiple bit upsets, latchup and for increasing total dose hardness is very simple: four times area increase. Doesn’t sound nice, but no one said it would be easy. However, if you’re ready for compromises, Radiation Hardening by Design allows achieving any predetermined level of radiation hardness at any bulk technology.
图8显示了65 nm批量技术中单事件翻转的实验数据。 左侧-常规商用6T-SRAM设计。 单打十下! 汉明代码无法保护您免受此类灾难的影响。 因此,当我们谈论商用IC时,粗制程节点要比较小的制程节点好一些,因为它们通常会更容易纠正单位位失调。 但是,当我们从头开始设计radhard芯片时,有大量的体系结构,原理图和布局解决方案能够产生高单事件容忍度和高性能。 图8的右侧还显示了来自6T-SRAM的结果,该结果来自相同的管芯,相同的原理图,但布局不同。 摆脱大多数多位打乱,闩锁和增加总剂量硬度的价格非常简单:面积增加四倍。 听起来不太好,但是没有人说这很容易。 但是,如果您准备妥协,则可以通过任意设计的辐射硬化设计,以任何预定的技术达到任何预定水平的辐射硬度。
Why predetermined? Because different requirements could be satisfied with different means. But why not apply all of them at once and be fine for every possible application? Most radiation hardening methods normally come at the cost of compromising functional parameters to some extent (supply current, area, speed, etc.). Therefore overengineering will lead to non-competitive products. Sure, such low-volume ICs are rarely made for just one application and should be flexible, but detailed and reasonable radiation requirements are absolutely vital for the successful design.
为什么要预定? 因为用不同的方法可以满足不同的要求。 但是,为什么不一次全部应用它们,并适合每种可能的应用呢? 通常,大多数辐射硬化方法都会以某种程度损害功能参数(电源电流,面积,速度等)为代价。 因此,过度设计将导致产品缺乏竞争力。 当然,这样的小批量集成电路很少会只为一种应用而制造,而是应该具有灵活性,但是详细而合理的辐射要求对于成功的设计绝对至关重要。
The eye of the attentive reader could’ve caught the word “bulk” in the phrase “predetermined level of radiation hardness at any bulk technology”. Isn’t it superfluous there? Isn’t it even wrong? It’s widely supposed that all the best radhard ICs are fabricated using “silicon on insulator” or “silicon on sapphire” technology. Right?
细心的读者可以在“任何批量技术中的预定辐射强度水平”一词中发现“散装”一词。 那里不是多余的吗? 甚至不对吗? 人们普遍认为,所有最好的radhard IC都是使用“绝缘体上的硅”或“蓝宝石上的硅”技术制造的。 对?
The “silicon on insulator” technology has long been firmly entrenched with “inherently radiation-hard” fame. The roots of this popular fallacy go back into antiquity, when its predecessor, SOS (silicon on sapphire) was actively used for military designs. Why? Transistors in SOS/SOI are electrically separated from each other and from the substrate. This means much lower radiation-induced charge collection volume, which is quite handy for dealing with high dose rate events as it significantly reduces the chip shutdown time right after the nearby nuclear explosion — indeed an important trait for a product designed during the Cold War.
长期以来,“绝缘体上的硅”技术已经以“固有的抗辐射性”声名远扬。 这种流行谬论的根源可以追溯到上古时代,当时其前身SOS(蓝宝石上的硅)被积极地用于军事设计。 为什么? SOS / SOI中的晶体管相互之间以及与基板之间均电隔离。 这意味着辐射引起的电荷收集量要低得多,这对于处理高剂量率事件非常方便,因为它可以显着减少附近核爆炸后的芯片关闭时间,这对于冷战期间设计的产品而言确实是一个重要特征。
Another part of the “SOI = Radhard” myth is insensitivity to latchup, including dose rate latchup. Latchup (also known as “thyristor effect”) is one of the main headaches for spaceborne systems’ designers as it’s unpredictable and catastrophic. So the technology allowing to deal with it for free could be naturally considered a heavens’ gift. But the whole picture is a little bit more complicated.
“ SOI = Radhard”神话的另一部分是对闩锁不敏感,包括剂量率闩锁。 闩锁(也称为“晶闸管效应”)是星载系统设计人员的主要难题之一,因为它不可预测且具有灾难性。 因此,允许免费处理的技术自然可以视为天赐之礼。 但是整个情况要复杂一些。
Figure 9. CMOS technology cross-section with parts of parasitic thyristor causing the latchup.
图9. CMOS技术截面图,其中部分寄生晶闸管引起闩锁。
The cause of the latchup effect is the parasitic thyristor structure present in bulk CMOS technology. If the resistances Rs and Rw are large enough, a hit of an ionizing particle can deposit enough charge to open parasitic thyristor and create a short between supply and ground. How big are these resistances in real chips? The answer is quite simple: contact to substrate or well means an extra area, so their number is usually minimized to make chips cheaper. This means that a random commercial IC is more likely to be vulnerable to latchup than not. Latchup, however, can occur not just after an ion strike, but also due to ESD, high temperature, excessive current density or a door being shut in the nearby room, so automotive and industrial IC designers are familiar with the topic and more likely to take measures against it.
闩锁效应的原因是体CMOS技术中存在的寄生晶闸管结构。 如果电阻Rs和Rw足够大,则电离粒子的撞击会沉积足够的电荷来打开寄生晶闸管,并在电源和地之间造成短路。 这些电阻在实际芯片中有多大? 答案很简单:与基板或Kong的接触意味着额外的面积,因此通常将其数量最小化以使芯片更便宜。 这意味着,随机商用IC更有可能遭受闩锁攻击。 但是,闩锁不仅可能发生在离子撞击之后,还可能由于ESD,高温,过大的电流密度或附近房间的门被关闭而引起,因此汽车和工业IC设计人员很熟悉该主题,并且更有可能这样做。采取措施。
A chip can be driven off of the latchup condition by supply reboot, and such a reboot is quite acceptable in many space applications, so many commercial products can still be used in space — even if with some caution. So-called latchup current limiters are very popular in radhard systems, especially in ones requiring high computational performance impossible with up-to-date radhard processors. But such a solution has many limitations. Power reset is not always possible as there is no shortage in real-time calculations. The reboot during an important manoeuvre can put an end to a long mission. The current consumption of a modern IC may vary in a few orders of magnitude according to its working mode, so current consumption in the “nothing happens and there is a latch” state may be less than in high-performance normal condition. Where to set the current limit for such a chip? The required system reaction time also depends on a protected chip as some of them are very vulnerable and others can sustain thousands of latchups if they are being reset sufficiently fast.
可以通过重新启动电源来使芯片脱离闩锁状态,并且这种重新启动在许多航天应用中是完全可以接受的,因此即使有一些谨慎,仍然可以在航天中使用许多商用产品。 所谓的闩锁电流限制器在radhard系统中非常流行,尤其是在那些需要最新radhard处理器无法实现的高计算性能的系统中。 但是这种解决方案有很多局限性。 并非总是可以进行电源重置,因为实时计算并不缺乏。 在重要的演习中重新启动可能会结束漫长的任务。 现代IC的电流消耗可能会根据其工作模式而在几个数量级上变化,因此“什么也没有发生并且有闩锁”状态的电流消耗可能会比高性能正常情况下的电流消耗少。 在哪里设置这种芯片的电流限制? 所需的系统响应时间还取决于受保护的芯片,因为其中一些芯片非常容易受到攻击,而如果它们被足够快地复位,则其他芯片可以承受数千个闩锁。
If a chip is fabricated on SOI technology, all these problems are not a concern anymore. And no protection circuitry is necessary — completely nothing. That’s why commercial SOI chips are so attractive for space applications. For example, the new American spacecraft Orion is controlled by a commercial SOI-based microprocessor PowerPC 750 rather than its radhard version RAD 750.
如果采用SOI技术制造芯片,那么所有这些问题都不再是问题。 无需保护电路-完全不需要。 这就是为什么商用SOI芯片在太空应用中如此具有吸引力的原因。 例如,新型美国航天器Orion由商用的基于SOI的微处理器PowerPC 750而不是其radhard版本RAD 750控制。
Figure 10. Leakage paths in bulk CMOS technology. Taken from J. Schwank et al., «Radiation effects in MOS oxides», IEEE Transactions on Nuclear Science, Vol. 55, No. 4, 2008
图10.批量CMOS技术中的泄漏路径。 摘自J. Schwank等人的《 MOS氧化物中的辐射效应》,IEEE Transactions on Nuclear Science,第1卷。 55,第4号,2008年
Then what’s the problem? There is not just a latchup, but also other radiation effects, and SOI is not inherently better than bulk technology in terms of both TID and SEE hardness. Figure 10 shows two leakage paths in bulk CMOS technology. Both of these paths are easily closed with proper layout design — one using ring n-channel transistors, the second — with the help of guard rings. These solutions have drawbacks from the point of view of the functioning of the circuit (restrictions on the minimum size of the ring transistor, area loss when using guard rings), but from the point of view of ensuring radiation resistance, they are very effective.
那是什么问题 不仅存在闩锁问题,还存在其他辐射影响,并且就TID和SEE硬度而言,SOI并非天生比本体技术更好。 图10显示了批量CMOS技术中的两条泄漏路径。 这两种路径都可以通过适当的布局设计轻松闭合-一种是使用环形n沟道晶体管,另一种是在保护环的帮助下。 从电路的功能的观点来看,这些解决方案具有缺点(限制环形晶体管的最小尺寸,使用保护环时的面积损失),但是从确保抗辐射性的观点来看,它们是非常有效的。
Figure 11. SOI buried oxide leakage path. Taken from J. Schwank et al., "Radiation effects in MOS oxides", IEEE Transactions on Nuclear Science, Vol. 55, N.4, 2008
图11. SOI掩埋氧化物泄漏路径。 取自J. Schwank等人,“ MOS氧化物中的辐射效应”,IEEE Transactions on Nuclear Science,第1卷。 55,N.4,2008
In SOI technology, there is another leakage path from the source to the drain along the boundary of silicon and latent oxide. Hidden oxide is much thicker than the gate, which means that it can accumulate a lot of positive charge. If we consider the "lower" transistor (the right part of Figure 11), for which the hidden oxide is a gate, we will see that in a normal situation, the source-gate voltage of this transistor is zero and its threshold voltage is several tens of volts, i.e. the current through this transistor does not flow. When irradiated, a positive charge is accumulated in the hidden oxide (this process is influenced by the geometry of the main transistor, in particular, by the thickness of the silicon instrument layer), and the threshold voltage of the “lower” n-channel transistor drops. As soon as it falls below zero, the current begins to flow freely through the transistor along the uncontrolled bottom channel. Thus, from the point of view of the total absorbed dose, the SOI technology is fundamentally strictly worse than the volumetric technology. But maybe there is a way to fix the situation somehow?
在SOI技术中,沿着硅和潜在氧化物的边界从源极到漏极还有另一条泄漏路径。 隐藏的氧化物比栅极厚得多,这意味着它可以积累很多正电荷。 如果我们考虑“下层”晶体管(图11的右半部分),其中隐藏的氧化物是栅极,我们将看到,在正常情况下,该晶体管的源极-栅极电压为零,而其阈值电压为几十伏,即不流过该晶体管的电流。 受到辐射时,正电荷会在隐藏的氧化物中积累(此过程受主晶体管的几何形状,特别是硅仪器层的厚度的影响)和“下部” n沟道的阈值电压晶体管滴。 一旦降到零以下,电流就开始沿着不受控制的底部通道自由流过晶体管。 因此,从总吸收剂量的角度来看,SOI技术从根本上说比体积技术要差。 但是也许有某种方法可以解决这种情况?
The substrate is usually grounded (in fact, connected to the lowest available potential), but in SOI nothing prevents us from setting negative voltage there and closing that parasitic back gate. This idea is, in fact, actively used — and in FDSOI technologies active back gate control is even used in their normal operation to minimize leakages in low-power modes and maximize speed when necessary. However, there is a catch: when we apply a high electric field to the buried oxide, we don’t just close the back transistor, but also accelerate the accumulation of positive charge. As a result, depending on technology specifics and the magnitude of the voltage applied, it’s possible that the total dose hardness will become even worse! There are other details, but in general, it’s possible to achieve almost any TID hardness level using standard CMOS technology, but there are some fundamental limitations for SOI. These limitations are normally negligible for low-orbit space applications, but if we’re speaking about multi-Megarad levels that could be present in the nuclear industry, commercially unfeasible technology changes are necessary for SOI.
基板通常接地(实际上,已连接到最低可用电位),但是在SOI中,没有什么可以阻止我们在此处设置负电压并关闭该寄生背栅。 实际上,这个想法已经得到了积极的运用,并且在FDSOI技术中,主动背栅控制甚至在其正常操作中也被使用,以最小化低功耗模式下的泄漏并在必要时最大化速度。 但是,有一个陷阱:当我们向埋入的氧化物施加高电场时,我们不仅会关闭后晶体管,还会加速正电荷的积累。 结果,取决于技术细节和所施加电压的大小,总剂量硬度可能会变得更糟! 还有其他细节,但总的来说,使用标准CMOS技术可以达到几乎任何TID硬度水平,但是SOI有一些基本限制。 这些限制对于低轨道空间应用通常可以忽略不计,但是如果我们谈论的是核工业中可能存在的多梅加拉德水平,那么SOI必须进行商业上不可行的技术变革。
Single event upsets in SOI are no less interesting. On the one hand, the charge collection volume in SOI is much smaller (although there is a long-lasting argument about the exact shape of this volume and its possible connection to the bulk). This means that we get less excessive charge and can dissipate it through supply lines faster, increasing chances of logic masking in cases on non-memory cells being hit.
SOI中的单事件失败也同样有趣。 一方面,SOI中的电荷收集体积要小得多(尽管对此体积的确切形状及其与主体的可能连接存在长期争论)。 这意味着我们得到的过量电荷更少,并且可以更快地通过电源线进行耗散,从而在非内存单元被击中的情况下增加了逻辑屏蔽的机会。
On the other hand, this small area has small capacitance, so even a small deposited charge can raise the voltage and open a parasitic bipolar transistor consisting of source, body and drain. If it happens, the deposited charge is multiplied by the gain of this parasitic transistor. In practice, this means threshold LET drop to levels below 1 MeV * cm ^ 2/(mg), and then effectively any incoming particle will cause a bit upset.
另一方面,这个小区域的电容很小,因此即使很小的沉积电荷也可以提高电压并打开由源极,基极和漏极组成的寄生双极晶体管。 如果发生这种情况,则所沉积的电荷将乘以该寄生晶体管的增益。 实际上,这意味着阈值LET降至低于1 MeV * cm ^ 2 /(mg)的水平,然后有效地,任何进入的粒子都会引起一点不安。
This negative effect, of course, could be mitigated by the careful low-ohmic connection between the transistor body and a respective power bus (or, in some cases, transistor source). But no one does this in commercial chips as these connections take a lot of areas and do nothing in exchange. Even in a radhard chip losing some area in each transistor can be a significant downside compared to bulk alternatives where one contact per 4-8 memory cells is often sufficient to prevent both latchup and parasitic bipolar multiplication. Even some guard rings can be set up with smaller area loss.
当然,可以通过在晶体管主体与相应的电源总线(或在某些情况下为晶体管源)之间进行仔细的低欧姆连接来减轻这种负面影响。 但是没有人会在商业芯片中做到这一点,因为这些连接占据了很多领域,却无所作为。 与批量替代方案相比,即使在radhard芯片中,每个晶体管中损失一些面积也可能是一个重大的缺点,在批量替代方案中,每4-8个存储单元一个触点通常足以防止闩锁和寄生双极乘法。 甚至可以设置一些面积较小的保护环。
SOI gets another important advantage at small process nodes where dielectric isolation helps prevent multiple bit upsets from a single particle, but modern cells are so small that a single ion track can directly affect two of them. However, it’s still much better than 10-bit upsets seen in experiments with bulk technology.
SOI在小型Craft.io节点上获得了另一个重要的优势,在这些Craft.io中,电介质隔离有助于防止单个粒子发生多次位翻转,但是现代单元是如此之小,以至于单个离子轨迹可以直接影响其中两个。 但是,它仍然比批量技术实验中看到的10位翻转要好得多。
Summing things up, SOI is not “inherently radiation hardened”, but it has some significant advantages and disadvantages compared to traditional bulk technology. The advantages could be exploited for a great effect, while disadvantages should be mitigated with a proper design. But the same is also true for bulk technology, so the proper process choice is not as trivial as it may seem and should be taken seriously in every single project. One should deeply understand the application to achieve desired levels of radiation hardness without making the chip unnecessarily complicated and too expensive.
总结一下,SOI并不是“固有地辐射硬化”的,但是与传统的批量技术相比,它具有一些明显的优缺点。 可以充分利用这些优点,而通过适当的设计来减轻这些缺点。 但是对于批量技术来说也是如此,因此正确的过程选择并不像看起来那样琐碎,应该在每个项目中认真对待。 人们应该深刻理解该应用,以达到所需的辐射硬度水平,而不会使芯片变得不必要的复杂和昂贵。
Many engineers across the globe are working on the topic of radiation hardness, and it’s completely impossible to cover everything in one article, especially if it’s dedicated to a wider audience. So, my colleagues will probably find enough oversimplifications or even mistakes, which I will be happy to discuss and correct. While not trying to be exhaustive, I hope that I gave my readers a brief understanding of what radiation hardening of electronic circuits is and that I was able to dispel some related misconceptions. Microelectronics in general and its special applications are one of the fastest evolving fields of applied science, so common knowledge becomes outdated very fast, while simple recipes are not used just because they don’t exist anymore.
全球许多工程师都在研究辐射硬度这一主题,并且完全不可能在一篇文章中涵盖所有内容,尤其是当它面向更广泛的受众时。 因此,我的同事们可能会发现足够的过度简化甚至错误,我将很乐于讨论和纠正。 尽管我不想穷尽所有,但我希望我能使读者对电子电路的辐射硬化有一个简要的了解,并希望我能够消除一些相关的误解。 总体而言,微电子学及其特殊应用是应用科学领域发展最快的领域之一,因此,常识变得非常过时,而不再使用简单的食谱,因为它们不再存在。
翻译自: https://habr.com/en/post/518366/
数字集成电路面试常见问题