Let\u2019s start first by explaining the problem itself, and then let\u2019s go back to the original tests we learned how to perform in an effort to make sense of the situation.<\/p>\n
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Many different classes of objects and measurements are used to determine the relationship between distance to an object and its apparent speed of recession that we infer from its light\u2019s relative redshift with respect to us. As you can see, from the very nearby Universe (lower left) to distant locations more than 10 billion light-years away (upper right), this very consistent redshift-distance relation continues to hold.\n<\/p>\n
Credit<\/a>: A.G. Riess et al., Astrophysical Journal, 2022<\/p>\n The problem is this: we know the Universe is expanding, and we\u2019ve been able to measure the expansion rate very well in recent years. Even given the puzzle<\/a> of the Hubble tension<\/a>, where fundamentally different methods yield answers that disagree at the 9% level, everyone agrees that the modern expansion rate of the Universe is somewhere between 67 and 74 km\/s\/Mpc. (Where 1 Mpc = 1 megaparsec = 3.26 million light-years.) To be conservative, we can split the difference and say the expansion rate is approximately 70 km\/s\/Mpc. This means, for a galaxy at any given distance, we can predict what its recession velocity is going to be through that simple relation: v = Hr.<\/p>\n For a galaxy 100 Mpc (326 million light-years) away, that\u2019s a recession speed of 7000 km\/s.<\/p>\n For a galaxy 1000 Mpc (3.26 billion light-years) away, that\u2019s a recession speed of 70,000 km\/s.<\/p>\n For a galaxy 4280 (14 billion light-years) Mpc away, that\u2019s a recession speed of 300,000 km\/s: the speed of light.<\/p>\n And for a galaxy at the distance of MoM-z14, 10,400 Mpc (33.8 billion light-years) away, that\u2019s a recession speed that equals 728,000 km\/s, or more than double the speed of light.<\/p>\n Clearly, something\u2019s wrong already. There\u2019s no way that an object, any object, can move through space at speeds that exceed the speed of light. According to the rules of Einstein\u2019s relativity, only massless objects can even reach the speed of light; objects with mass can only approach it from below, never reaching or exceeding it, no matter how much energy you put into it or how long you accelerate for.<\/p>\n These four graphs, all part of the same calculation but shown on different timescales, show how accelerating at \u201c1 g,\u201d or the gravitational acceleration on Earth, would lead to your velocity increasing and (eventually) approaching the speed of light relative to a stationary observer back on Earth. Note that you can never quite reach the speed of light, no matter how long you accelerate for.\n<\/p>\n Credit<\/a>: E. Siegel<\/p>\n You might think to yourself, \u201coh, of course, let\u2019s just apply special relativity to this!\u201d After all, the way we infer a galaxy\u2019s recession speed is to look at the shift of its spectral lines towards longer wavelengths: a redshift. This lengthening effect happens all the time for all sorts of waves, not just light.<\/p>\n If you have a regular series of waves in the water, if you move in the same direction as the waves, each one will take longer to pass and overtake you. If you move at the same speed as the waves, they\u2019ll never overtake you at all.<\/p>\n If you have a sound being emitted from a siren, if you move away from the emitting source, the sound waves will take longer to pass by you, lengthening the wavelength of the sound you hear and lowering the pitch. If you move at the same speed as the waves \u2014 the speed of sound \u2014 they\u2019ll never catch up to you, and you\u2019ll never hear them.<\/p>\n But if you have light being emitted from a source, when you move away from the emitting source, the light will still always move relative to you at the speed of light, no matter how fast you go. Its wavelength will lengthen, but the waves will still overtake you: you can never move fast enough so that the light won\u2019t catch you.<\/p>\n In other words, these severe redshifts that we\u2019re seeing can\u2019t be naively construed at moving at or faster than the speed of light; we\u2019d have to switch to doing relativistic calculations. Can that help us?<\/p>\n As the diagram shows, the closer you move to the speed of light (top panel), the more severely incoming light gets blueshifted in your direction of motion, while the more severely redshifted it gets in the direction away from your motion. This applies to any two objects dependent on their relative motion, regardless if it\u2019s the source, the observer, or both that are in motion.\n<\/p>\n Credit<\/a>: TxAlien\/English-language Wikipedia<\/p>\n If we apply the relativistic Doppler effect<\/a>, instead of the classical recession velocities we applied earlier, we\u2019d get somewhat different speeds for the same galaxies we considered earlier. Only this time, instead of distance, I\u2019m going to display their redshift, and what recession speed that translates into given that same expansion rate, today, of 70 km\/s\/Mpc.<\/p>\n For a galaxy at redshift z = 0.0233, that\u2019s a recession speed of 6900 km\/s.<\/p>\n For a galaxy at redshift z = 0.233, that\u2019s a recession speed of 62,000 km\/s.<\/p>\n For a galaxy at redshift z = 1.414, that\u2019s a recession speed of 212,000 km\/s: 71% the speed of light.<\/p>\n And for a galaxy at MoM-z14\u2019s redshift, z = 14.44, that\u2019s a recession speed of 297,300 km\/s: 99.2% the speed of light.<\/p>\n This time, nothing is moving faster than the speed of light, as we used special relativity to transform the observed redshift into the corresponding difference between the velocities of the source and the observer.<\/p>\n It\u2019s this line of thinking that leads to questions like the one we\u2019re considering here: how did these objects acquire such great velocities? Where did they get the energy to be moving away so quickly? If this applies to all of the distant, high-redshift galaxies we observe, does this mean something\u2019s wrong with physics for our understanding of the Universe?<\/p>\n I will note that the problem isn\u2019t necessarily with viewing the recession as a Doppler shift; it can be done properly<\/a>, although when most people try, it often leads to confusion. The problem is viewing it from a special relativistic perspective. To make sense of it, we have to think from a general relativity perspective, instead.<\/p>\n An animated look at how spacetime responds as a mass moves through it helps showcase exactly how, qualitatively, it isn\u2019t merely a sheet of fabric. Instead, all of 3D space itself gets curved by the presence and properties of the matter and energy within the Universe. Space doesn\u2019t \u201cchange shape\u201d instantaneously, everywhere, but is rather limited by the speed at which gravity can propagate through it: at the speed of light. The theory of general relativity is relativistically invariant, as are quantum field theories, which means that even though different observers don\u2019t agree on what they measure, all of their measurements are consistent when transformed correctly.\n<\/p>\n Credit<\/a>: LucasVB<\/p>\n The biggest differences between special relativity and general relativity are as follows.<\/p>\n In special relativity, spacetime is a fixed, static background. It is flat, with no curvature, and doesn\u2019t evolve over time based on what\u2019s in that spacetime.<\/p>\n In general relativity, spacetime is a changing, dynamic background. It can be flat, positively curved, or negatively curved, and must evolve over time in a fashion that\u2019s dependent on what the different forms of energy are within it, as well as how that energy is distributed.<\/p>\n If you only viewed our Universe from the perspective of special relativity, then it would be impossible for any object to be farther away than 27.6 billion light-years today. Remember, our Universe is 13.8 billion years old, as measured since the start of the hot Big Bang. Even if you began with an object that was 13.8 billion light-years away and moving away from us at 99% or more of the speed of light, then today, when that light arrives, that object would only be at a maximum distance of double that figure: 27.6 billion light-years.<\/p>\n But that is not how distances work in a universe governed by general relativity, and we have two different measurable things we can use to demonstrate that many distant galaxies \u2014 including MoM-z14 \u2014 are not only more distant than they would be in a universe governed by special relativity, but that are even farther away than that 27.6 billion light-year limit set by a special relativistic universe.<\/p>\n This annotated, rotated image of the JADES survey, the JWST Advanced Deep Extragalactic Survey, shows off the first galaxy of the JWST era to hold the cosmic distance record: JADES-GS-z13-0, whose light comes to us from a redshift of z=13.2 and a time when the Universe was only 320 million years old. This galaxy appears about twice as large, in terms of angular diameter, as it would appear if it were half the distance away: a counterintuitive consequence of our expanding Universe.\n<\/p>\n Credit<\/a>: NASA, ESA, CSA, M. Zamani (ESA\/Webb); Science credits: Brant Robertson (UC Santa Cruz), S. Tacchella (Cambridge), E. Curtis-Lake (UOH), S. Carniani (Scuola Normale Superiore), JADES Collaboration; Annotation: E. Siegel<\/p>\n One test we can perform is to measure a distant galaxy\u2019s angular diameter: how large, in terms of degrees, arcminutes, arcseconds, or fractions-of-an-arcsecond, does an observed object take up on the sky? You might think, if you took a galaxy and moved it twice as far away, it would take up just one-half of its original angular diameter. If you moved it ten times as distant, it\u2019d be one-tenth the original size. And if you moved it a thousand times as far away as it was initially, you\u2019d see it as just one-thousandth of its original angular size. This is just straightforward geometry, after all.<\/p>\n But that reasoning only applies to a special relativistic spacetime: one that doesn\u2019t curve, expand, or otherwise evolve with time. In general relativity, however, an expanding universe leads you to a very different picture. As you move an object farther away from you, its angular diameter initially decreases as it would in a special relativistic spacetime: inversely proportional to its distance. However, at a certain point several billion light-years away, that decrease would slow and slow, eventually reaching a minimum angular size. Beyond that distance, the angular diameter grows again, meaning that if we can measure an object\u2019s size at a given distance, we should be able to tell these two cases or interpretations apart.<\/p>\n The way that light spreads out as a function of distance means that the farther away from a power source you are, the energy that you intercept drops off as one over the distance squared. This also illustrates, if you view a certain specific angular area (illustrated by the squares) from the perspective of the original source, how larger objects at greater distances will appear to take up the same angular size in the sky. Each time you double your distance between a source and observer, the brightness you observe gets quartered. In general, photons (and all light) propagate spherically outward away from the emitting source.\n<\/p>\n Credit<\/a>: Borb\/Wikimedia Commons<\/p>\n A second test we can conduct is to measure an object\u2019s apparent brightness: how bright it appears to our eyes, telescopes, and instruments. In our everyday lives, we can see that brightness just falls off as shown above: as one over the distance squared, because light signals spread out in a sphere when they\u2019re emitted from a source. An observer on Jupiter, five times as far away as the Earth is from the Sun, sees the Sun as just one-twenty-fifth as bright as a terrestrial observer would, while an observer on Neptune, thirty times as distant as on Earth, sees the Sun to be just one-nine-hundredth as bright.<\/p>\n But in our expanding Universe, the relationship is more complicated (dependent on additional factors that involve the object\u2019s redshift) than it is in the naive, special relativistic picture. The farther away you bring an object, the fainter it appears, but at great distance, it appears brighter than the naive expectation. This is not just different than the naive expectation, but it\u2019s also different from the angular diameter distance relationship.<\/p>\n This means that if you can:<\/p>\n know an object\u2019s intrinsic size and brightness,<\/p>\n measure how bright that object appears (its apparent luminosity),<\/p>\n measure how large that object appears (its apparent angular size),<\/p>\n and compare their inferred distances,<\/p>\n you can actually determine how the Universe behaves, whether it\u2019s expanding or not, and what its properties and composition are.<\/p>\n Standard candles (left) and standard rulers (right) are two different techniques astronomers used to measure the expansion of space at various times\/distances in the past. Based on how quantities like luminosity or angular size\/diameter change with distance, we can infer the expansion history of the Universe. Standard candles involve looking at objects whose intrinsic brightness is known at all cosmic distances, while standard rulers involve looking at features such as the physical size of a known object or the average separation distance between any two galaxies (imprinted from baryon acoustic oscillations during the early stages of the Big Bang) that evolve as the Universe expands.\n<\/p>\n Credit<\/a>: NASA\/JPL-Caltech<\/p>\n Although it\u2019s a difficult task, we\u2019ve managed to accomplish it in a variety of ways with a large number of different distance indicators, albeit, for many of them, with large uncertainties.<\/p>\n One thing the data is definitive about, however, is how inconsistent these tests are with a special relativistic universe: where objects just get smaller according to one-over-the-distance or where they get fainter as one-over-the-distance-squared. For objects in the relatively nearby Universe \u2014 within around one billion light-years of us \u2014 these differences are small, and measurement would need to be extremely precise to accurately report those differences: to just a few percent precision. It\u2019s very difficult to get such accurate, precise estimates for individual objects, making such a determination difficult.<\/p>\n But at greater and greater distances, those differences become profound. At distances of around 10 billion light-years, the luminosity distance differs by more than a factor of two from the naive prediction. At those same distances, the angular diameter distance also differs by more than a factor of two from the naive prediction, but in the opposite direction. Even if we aren\u2019t using the same objects for luminosity distance and angular diameter distance, we can still use these measurements to teach us about the type of Universe that we live in, and to see what sorts of rules it obeys.<\/p>\n These graphs show, for low redshifts on a linear scale (left) and large redshifts on a logarithmic scale (right) how luminosity distance and angular diameter distance vary and differ from the naive (special relativistic) relationship between redshift and distance. The better we can constrain the redshift-distance relation, the better we can understand our expanding Universe and what governs it.\n<\/p>\n Credits<\/a>: Wesino\/English Wikipedia\/public domain<\/p>\n The reason this is so important is because this is what we can measure directly: the properties of objects like \u201chow bright do they appear\u201d or \u201chow large of a size do they take up?\u201d We can\u2019t measure the expanding Universe directly; we can only infer it.<\/p>\n What you\u2019d want to do is have a large collection of objects \u2014 the same class of object but with many examples of it \u2014 at different distances and redshifts, but where some intrinsic property of that object is well-known. One of the best-known examples in astronomy of such a phenomenon is type Ia supernovae. Now known to originate from the detonation of a white dwarf<\/a>, typically upon collision with another white dwarf, there\u2019s a well-known relationship between how intrinsically bright the supernova is and the time it takes that supernova to brighten, reach maximum brightness, and decline.<\/p>\n You can then infer the distance to that object based on how bright the object appears versus how intrinsically bright it is. When you also measure the object\u2019s redshift and do this for hundreds or even thousands of objects, you can construct a redshift-distance diagram. This allows you to conclude what\u2019s in your Universe, how it\u2019s expanding, and whether it\u2019s obeying the rules of special relativity, general relativity, or something else entirely.<\/p>\n A plot of the apparent expansion rate (y-axis) vs. distance (x-axis) is consistent with a Universe that expanded faster in the past, but where distant galaxies are accelerating in their recession today. This is a modern version of, extending thousands of times farther than, Hubble\u2019s original work. Note the fact that the points do not form a straight line, indicating the expansion rate\u2019s change over time. The fact that the Universe follows the curve it does is indicative of the presence, and late-time dominance, of dark energy.\n<\/p>\n Credit<\/a>: Ned Wright\/Betoule et al., 2014<\/p>\n We leverage this exact method, as well as several others just like it that take advantage of various distance indicators, to measure the distance to various objects, to determine the expansion history of the Universe, and to demonstrate that our Universe isn\u2019t consistent with a special relativistic perspective.<\/p>\n This last part is the most important. Once we recognize that we have to consider that:<\/p>\n spacetime isn\u2019t a fixed backdrop, but rather curves and evolves,<\/p>\n that objects don\u2019t just move through spacetime, but that spacetime itself expands,<\/p>\n and that what we perceive as an object\u2019s redshift is a combination of its motion through spacetime and the expansion of the Universe,<\/p>\n we can begin to make sense of both how far away objects are and how much of what we see as their redshift is and isn\u2019t due to their motion. For MoM-z14, the current cosmic record-holder<\/a>, we can determine that it\u2019s approximately 33.8 billion light-years away from us right now: more than 6 billion light-years farther than the distance limit for a special relativistic universe. We can also say, for practically every object we can observe, that while they might have peculiar motions that cause them to move at hundreds or even thousands of km\/s relative to the Hubble flow, the majority of their observed redshift, particularly at large distances, is all due to cosmic expansion, and not to their motion through space. <\/p>\n This graph shows the differences between a cosmology consistent with general relativity and both dark matter and dark energy (solid, dark lines and shading), as compared with a purely special relativistic cosmology (where all of the speed is due to motion, rather than expanding space) or with the naive extrapolation of Hubble\u2019s law (v = cz line). The data clearly fits only the general relativistic interpretation.\n<\/p>\n![\"Four](\"https:\/\/www.newsbeep.com\/nz\/wp-content\/uploads\/2026\/05\/approach-c.jpg\")
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