宇宙中缺失的一半物质
直到最近,宇宙中仍有大约一半的物质处于缺失、隐藏或未被探测到的状态。
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Until recently, half the universe was missing or hidden or just... undetected.
不,我说的不是分别占据宇宙27%和68%的暗物质(Dark Matter: 一种不发光、不吸收光、不反射光,但能通过引力效应被探测到的物质)或暗能量(Dark Energy: 一种假想的能量形式,被认为导致宇宙加速膨胀)。
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And no, I'm not talking about dark matter or dark energy, which make up 27 and 68 percent of our universe, respectively.
我指的是构成你我、行星、恒星、星云以及基本上所有你可见事物的普通物质。
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No, I'm talking about normal ordinary matter Which makes up you and me and the planets and stars and nebulae, and basically everything you can see.
由于这些物质大多由质子和中子组成,而它们都是重子(Baryons: 由三个夸克组成的复合粒子,如质子和中子)的一种形式,因此这个问题被称为缺失重子问题(Missing Baryon Problem: 宇宙中观测到的重子物质少于理论预测量的问题)。
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And since most of this stuff is made of protons and neutrons, which are forms of baryons, this has been known as the missing baryon problem.
我们预计宇宙应由5%的重子物质(Baryonic Matter: 由重子构成的普通物质)组成。
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We expect the universe to be made up of 5 percent baryonic matter.
然而,当我们实际观测时,却只发现了2.5%。
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But when we go looking, we only find 2.5 percent.
为什么宇宙中应有5%的重子物质?
那么,你可能首先会问:“我们为什么会认为宇宙最初就应该含有5%的普通重子物质呢?”
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Now, the first question you're probably asking is "Why should we expect the universe to be 5 percent ordinary baryonic matter in the first place?"
答案是,有了这个密度,我们才能解释宇宙中观测到的各种元素的相对丰度。
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The answer is because, with that density, we can explain the relative abundances of different elements that we observe in the universe.
具体来说,就是氘(Deuterium: 氢的同位素,原子核含一个质子和一个中子)、氢(Hydrogen: 原子序数为1的元素)和氦(Helium: 原子序数为2的元素)的比例。
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Specifically, the ratio of deuterium to hydrogen to helium.
在宇宙诞生之初,也就是大爆炸(Big Bang: 宇宙起源的理论模型)之后,所有的中子和质子都在四处飞驰。
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In the beginning, like right after the Big Bang, there were all of these neutrons and protons whizzing around.
当时宇宙极度炽热,充满了大量的辐射。
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It was incredibly hot, and there was tons of radiation.
宇宙处于辐射主导时期。
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The universe was radiation dominated.
然而,随着宇宙的膨胀,它逐渐冷却,使得质子和中子能够开始聚变。
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But, as the universe expanded, it cooled to the point where protons and neutrons could start fusing together.
其中一种特别稳定的原子核是氦-4,由两个中子和两个质子组成。
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A particularly stable nucleus to form would be helium-4, made of two neutrons and two protons.
问题在于,要形成氦-4,首先必须形成氘,它由一个质子和一个中子构成。
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The problem was, to form helium-4, you first have to form deuterium, one proton and one neutron.
而氘是一种不太稳定的原子核,它刚一形成就会迅速被撞碎。
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And, this is a less stable nucleus. And as quickly as it formed, it would get smashed apart.
但是,在大爆炸发生约10秒后,宇宙已冷却到足以让氘形成的程度。
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But, by about 10 seconds after the big bang, the universe had cooled sufficiently that deuterium could form.
一旦形成,它就会迅速聚变为氦。
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And as soon as it did, it would rapidly fuse into helium.
这个过程的速度取决于早期宇宙中物质的密度。
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The rate at which this happened depended on the density of matter in the early universe.
密度越高,聚变发生的速度就越快。
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The higher the density - the faster this fusion could occur.
随后,在大爆炸发生约20分钟后,温度已降至聚变无法再进行的程度。
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Then, by 20 minutes after the Big Bang, the temperature had dropped low enough that fusion could no longer occur.
因此,在那个时刻,元素的丰度被固定下来,就像那一瞬间的快照。
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So, at this point, the elemental abundances were locked in. Like a snapshot of this moment.
按质量计算,宇宙中含有75%的氢和25%的氦。
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There were 75% hydrogen and 25% helium, by mass.
这基本上与我们今天在宇宙中观测到的情况一致。
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Which is basically still what we observe in the universe today.
在氢原子核中,每百万个就有26个是氘。
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Of the hydrogen nuclei, 26 out of every million were deuterium.
氘的奇妙之处在于它非常稳定,不会衰变。
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What's amazing about deuterium is that it's stable - it doesn't decay.
而且,自大爆炸以来,没有已知的过程能够大量产生它。
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And there are no known processes that can produce it in significant quantities since the Big Bang.
这意味着,今天宇宙中几乎所有的氘,包括自来水中每6000个氢原子中就有一个氘原子,都不是在恒星中产生的,而是在大爆炸后的最初20分钟内形成的。
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And that means, virtually all the deuterium in the universe today, including the one out of every 6000 hydrogen atoms in tap water was created not in stars but in the first 20 minutes after the Big Bang.
当我们深入太空观测时,所能看到的最古老的光是宇宙微波背景辐射(Cosmic Microwave Background Radiation: 大爆炸后遗留至今的微弱电磁辐射)。
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When we look deep into space, the oldest light we can see is the Cosmic Microwave Background Radiation.
这种大爆炸的余晖,自大爆炸后约40万年以来,便一直畅通无阻地穿梭于宇宙之中。
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The afterglow of the big bang which has been traveling through the universe unimpeded since about 400,000 years after the Big Bang.
因此,我们能够精确地计算这些光子,并推算出大爆炸后辐射的密度。
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And so we can literally count up those photons and work out the density of radiation right after the Big Bang.
利用每百万个氢原子核中有26个氘原子核的数值,我们就能计算出重子物质与光子的比例,从而推断出宇宙中应该含有大约5%的重子物质。
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And using the value of 26 deuterium nuclei per million hydrogen nuclei, well, we can work out the ratio of baryonic matter to photons, and that is how we work out that there should be about five percent baryonic matter in the universe.
寻找缺失的重子:类星体与莱曼-阿尔法森林
因此,在1990年代后期,科学家们开始寻找所有这些重子物质。
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So in the late 1990s scientists went looking for all this baryonic matter.
这就像是一次普查。
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It was a census of sorts.
他们统计了所有的行星、恒星、黑洞、星系、尘埃云和气体,基本上是所有能通过望远镜看到或推断存在的事物。
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They added up all of the planets and stars and black holes, galaxies, dust clouds, gas, basically everything you can see or infer exists using a telescope.
他们发现,我们通常认为构成宇宙实际物质的一切,仅仅占所有重子物质的不到20%。
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And what they found is that everything that I normally think of as the actual stuff in our universe, it only makes up barely 20 percent of all the baryonic matter.
那么,其余的物质在哪里呢?
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So where is the rest?
并非所有普通物质都会明亮发光或被附近的恒星照亮。它不是暗物质,但它确实是处于黑暗中的普通物质。
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Well, not all ordinary matter is glowing brightly or is illuminated by nearby stars It's not dark matter but it is ordinary matter that is just in darkness.
因此,如果想找到这些重子,一种方法是使用背景光——一个来自非常遥远、也就是早期宇宙的明亮光源。
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And so if you want to find those baryons, well, one way is to use a backlight -- a bright source of light very far away, and that also means in the very early universe.
类星体(Quasars: 宇宙中最明亮、最遥远的天体之一,通常由星系中心的超大质量黑洞吸积物质产生)就是完美的背景光。
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And quasars are the perfect backlight.
它们的亮度可以是整个星系的数千倍。
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Their luminosity can be thousands of times that of whole galaxies.
这些光来自早期星系中心超大质量黑洞的吸积盘,当它吞噬周围物质时便会发光。
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The light comes from the accretion disk of a supermassive black hole at the center of an early galaxy as it engulfs all this matter.
由于它们距离如此遥远,我们从类星体接收到的光会严重红移(Redshifted: 光谱线向波长较长的红色端移动的现象,通常表示光源正在远离观测者)。
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And since it is so distant the light we receive from quasars is heavily redshifted.
例如,当氢原子从第一激发态跃迁到基态时发出的光——即莱曼-阿尔法跃迁(Lyman-alpha Transition: 氢原子从第一激发态跃迁到基态时发出的特定波长的光)——在实验室中会产生波长约为121.6纳米的紫外光。
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For example, the light emitted when a hydrogen atom goes from its first excited state to its ground state, the Lyman-alpha transition, it produces ultraviolet light of around 121.6 nanometers in a lab.
但从类星体发出的这种光,在光谱中可以观测到超过560纳米的峰值——也就是黄光。
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But from a quasar it can be observed as a peak in their spectrum at over 560 nanometers -- that is yellow light.
令人着迷的是,如果你观察这个峰值的左侧,你会看到许多小小的凹陷。
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What's fascinating is if you look to the left of this peak you see many little dips.
这些是位于我们与类星体视线方向上的中性氢原子所产生的吸收线。
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These are absorption lines created by neutral hydrogen atoms that lie along our line of sight with the quasar.
当类星体发出的光遇到中性氢时,那些能够激发电子从基态跃迁到第一激发态的光子就会被吸收。
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When light from the quasar reaches neutral hydrogen the photons that can excite the electrons from the ground state to the first excited state are absorbed.
这同样是莱曼-阿尔法跃迁,但由于这些氢气团离我们更近,它们的红移程度较小,因此它们在光谱中形成的凹陷,离我们越近的气体,其波长就越短。
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This is the same Lyman-alpha transition, but since these patches of hydrogen gas are closer to us they are less redshifted so the notches they make in the spectrum are at shorter and shorter wavelengths the closer the gas is to us.
这种现象被称为莱曼-阿尔法森林(Lyman-alpha Forest: 类星体光谱中由沿视线方向的中性氢吸收线形成的复杂图案)。
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This has been described as the Lyman-alpha forest.
它就像一张一维地图,向我们展示了沿着连接我们与类星体的视线方向上,中性氢气体的分布位置和数量。
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It's like a one-dimensional map that shows us where and how much neutral hydrogen gas lies along the line connecting us to the quasar.
将所有这些中性氢气体纳入我们的重子预算后,我们找到了近50%的缺失重子。
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Adding all of that neutral hydrogen gas into our baryon budget brings us almost to 50 percent.
温热星系际介质(WHIM):重子的藏身之处
那么,另一半重子在哪里呢?
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So where is the other half of the baryons?
宇宙的计算机模拟表明,它们分布在星系之间的薄片或纤维状结构中,并且非常稀疏——每立方米只有一到十个粒子。
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Well, computer simulations of the entire universe suggested they are out there just in between the galaxies in these sheets or filaments and they're very spread out -- just one to ten particles per cubic meter.
此外,这些粒子是电离(Ionized: 原子或分子失去或获得电子而带电荷的过程)的,所以它们不像中性氢气那样吸收光线。
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Plus, these particles are ionized so they don't absorb the light like the neutral hydrogen gas.
它们的温度介于约10万到1000万开尔文之间,天文学家称之为温热范围,因此这被称为温热星系际介质(Warm-Hot Intergalactic Medium: 存在于星系之间,温度介于10万到1000万开尔文的稀薄电离气体),简称WHIM。
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And they're in a temperature range between about 100,000 and 10 million Kelvin, a range astronomers like to refer to as warm-hot, so this is known as the warm-hot intergalactic medium or WHIM for short.
但寻找WHIM一直是个真正的挑战,因为它们是电离的,并且由于其温度,它们只在高能紫外线或低能X射线波段发射或吸收。
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But finding the WHIM has been a real challenge because they're ionized, because of their temperature, they only emit or absorb in the high energy UV or low energy X-rays.
虽然有些人曾使用非常复杂的技术试图找到WHIM,但最近,一种自然发生的物理现象使我们得以找到所有缺失的重子。
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Now, some people have used very sophisticated techniques to try to find the WHIM but then recently a naturally occurring physical phenomenon allowed us to find all of the missing baryons.
让我们来看看是如何做到的。
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Let's find out how.
快速射电暴:揭示缺失重子的关键
首先,我们需要谈谈闪电,我保证这与主题相关。
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First we need to talk lightning and I promise this is related.
那么,你知道从地球的另一端也能探测到闪电吗?
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Okay so did you know that it's possible to detect lightning from the other side of the earth?
这是因为闪电会在电磁波谱的所有部分产生电磁辐射闪光。
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This is because lightning produces a flash of electromagnetic radiation in all parts of the spectrum.
我们能看到白光,但同时也会释放出广谱无线电波,如果你在附近,就能探测到它们以脉冲形式出现。
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I mean we see the white light but there's also broad spectrum radio waves which are released and if you were nearby you could detect those as a pulse.
然而,极低频无线电波实际上可以穿透大气层,沿着地球磁力线向外传播数个地球半径,然后再次返回地球,并在另一个半球被探测到。
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But the very low frequency radio waves can actually travel up and out of the atmosphere and they get guided along the Earth's magnetic field lines out several radii from the Earth and then back down where they can be detected in the other hemisphere.
但如果它们在那里被探测到,它们不会以单一脉冲的形式出现,而是会分散成一种啸叫声(whistler)。
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Except if they're detected there they don't come in as a single pulse, instead they are spread out as a whistler.
现在,如果你通过扬声器播放这些无线电波,我们实际上可以听到它们,请听。
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Now if you play these radio waves through a speaker we can actually hear them, so listen to this.
你听到那种听起来像科幻激光枪的下降音调了吗?
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You hear that descending tone that sounds like a sci-fi laser gun?
是的,那就是地球另一端的闪电。
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Yeah, that is lightning on the other side of the earth.
那么,这里发生了什么?
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So what's happening here?
当无线电波穿过地球磁层时,它们会遇到自由电子,这会使它们减速,特别是对较低频率的波而言:这就是色散(Dispersion: 波在介质中传播时,其传播速度随频率变化的现象)。
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Well, as the radio waves travel through the earth's magnetosphere they encounter free electrons, which slows them down and more for the lower frequency waves: this is dispersion.
就像棱镜将白光分解成其组成颜色一样,磁层中的等离子体会将无线电波分解成其组成频率:低频波比高频波减速更多,因此最初的脉冲最终会变成啸叫声。
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Just as a prism separates white light into its component colors the plasma in the magnetosphere separates the radio waves into its component frequencies: low frequencies are slowed down more than high frequencies, so what started as a pulse ends up as a whistler.
色散的程度会告诉你,该无线电波在到达探测器之前穿过了多少自由电子。
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And the amount of dispersion tells you how many free electrons that radio wave had to pass through to reach the detector.
现在,想象一下我们能够做类似的事情来寻找宇宙中所有电离的重子。
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Now just imagine we could do something very similar to find all the ionized baryons in the universe.
我们所需要的,只是宇宙深处某个地方发出的明亮无线电闪光。巧合的是,在2007年,天文学家发现了第一个快速射电暴(Fast Radio Burst, FRB: 持续时间极短但强度极高的射电脉冲),顾名思义,它就是一种持续时间极短的强烈无线电波脉冲。
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All we would need is a bright flash of radio waves somewhere in the distant universe and as if on cue in 2007 astronomers found the first fast radio burst, which is just what it sounds like: a very short-duration pulse of intense radio waves.
它来自遥远的宇宙深处,来自其他星系。
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And it came from the deep universe, from other galaxies.
这些脉冲的威力极其巨大,可以达到太阳的数十亿甚至数万亿倍,但它们只持续约一毫秒。
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Now, these pulses can be incredibly powerful, I'm talking billions or trillions of times as powerful as the sun, but they last for on order of a millisecond.
我们尚不清楚它们是如何产生的,尽管有些人猜测它们可能由磁星(Magnetars: 具有极强磁场的中子星)或中子星(Neutron Stars: 大质量恒星坍缩后的致密残骸)产生,或是这些极其强大的大质量天体(如黑洞和中子星)之间的某种碰撞所致。
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We don't really know what creates them, though some people suspect that it's magnetars or neutron stars or some sort of collision between these very powerful massive objects like black holes and neutron stars.
但就我们的目的而言,我们只需要知道这些闪光的存在,并且我们可以利用它们来观察其色散,从而计算出我们与光源之间有多少电离重子。
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But for our purposes all we need to know is that those flashes exist and that we can use them to look at their dispersion and figure out how many ionized baryons are between us and the source.
这正是一篇近期发表在《自然》杂志上的论文所做的工作:他们绘制了几个快速射电暴的色散量(Dispersion Measure: 衡量电磁波穿过电离介质时色散程度的物理量)与其宿主星系红移的关系图。
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And this is exactly what one recent paper did in Nature: they plotted out the dispersion measure of several of these fast radio bursts versus the redshift of their host galaxy.
他们发现,果然,这些快速射电暴距离越远,其信号到达地球时的色散程度就越高。
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And what they found was, sure enough, the further out these fast radio bursts were the more dispersed their signal when it reached the earth.
事实上,利用他们的测量结果,他们能够估算出宇宙中存在的总重子物质,其中包括WHIM中的所有电离粒子,他们发现这个比例正是5%。
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And in fact using their measurements they were able to estimate the total baryonic matter that is out there, and that includes all the ionized particles in the WHIM, and they found that it was five percent.
他们找到了缺失的重子。大约50%的重子存在于温热星系际介质中,这证实了我们一直以来的设想。
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They found the missing baryons. Roughly 50 percent of them are in that warm-hot intergalactic medium and so this validates what we had been thinking the whole time.
科学的胜利与展望
你知道,制作这个视频时令我惊讶的是,我意识到大爆炸产生的普通物质中,只有极小一部分最终形成了恒星和星系——那些我通常认为是宇宙组成部分的东西。
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You know, what surprised me in making this video was realizing just how little of the ordinary matter from the big bang ended up in things like stars and galaxies, what I normally consider as the stuff of the universe.
不,那只占所有重子物质的10%到20%左右。
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No, that's only like 10 or 20 percent of all the baryonic matter.
所以,这些有趣结构的形成过程,实际上是一个非常低效的过程。
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So it turns out the formation of these interesting structures is a really inefficient process.
但这一发现是科学的又一次胜利。
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But this finding is yet another triumph for science.
几十年前进行的那些计算机模拟结果,在很大程度上被证明是正确的,因此所有参与者都应受到祝贺。
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Those computer simulations run decades ago turned out largely to be correct and so everyone involved should be congratulated.
但这对我来说也凸显了科学家和非科学家之间的区别。
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But this also highlights for me the difference between scientists and non-scientists.
我觉得非科学家喜欢正确,他们喜欢事情按预期发展。
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I feel like non-scientists like being right, they like when things turn out the way they were expecting,
但另一方面,科学家则希望事情不按预期发展,因为这正是我们获得线索,探索仍待发现的新物理学的方式。
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but scientists on the other hand, they want things to work out not the way they expected because that's the way we get clues into what new physics is still out there to be discovered.
我想目前我们只能满足于“正确”了。
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I guess for now we'll have to be content with being right.