{"id":601368,"date":"2026-04-13T14:47:23","date_gmt":"2026-04-13T14:47:23","guid":{"rendered":"https:\/\/www.newsbeep.com\/ca\/601368\/"},"modified":"2026-04-13T14:47:23","modified_gmt":"2026-04-13T14:47:23","slug":"one-bad-measurement-ruled-out-as-hubble-tension-explanation","status":"publish","type":"post","link":"https:\/\/www.newsbeep.com\/ca\/601368\/","title":{"rendered":"“One bad measurement” ruled out as Hubble tension explanation"},"content":{"rendered":"

For 15 years now, the expanding Universe hasn\u2019t added up<\/a>.<\/p>\n

\"\"<\/p>\n

This graph shows a comparison between the value of H0, or the expansion rate today, as derived from Hubble Space Telescope Cepheids and anchors as well as other subsamples of JWST Cepheids (or other types of stars) and anchors. A comparison to Planck, which uses the early relic method instead of the distance ladder method, is also shown. Very clearly, the distance ladder and early relic methods do not yield mutually compatible results.\n<\/p>\n

Credit<\/a>: A.G. Riess et al., Astrophysical Journal submitted, arXiv:2408.11770, 2024<\/p>\n

Different measurement methods should converge on the same answer<\/a>.<\/p>\n

\"A<\/p>\n

A large class of early relic methods, involving either the CMB and\/or BAO (with a specific focus on DESI publications), all favor a Universe expanding at ~67 km\/s\/Mpc. Although there are a few groups that have outlier values for distance ladder measurements (including the CCHP group, shown as the second-from-bottom point), the strongest measurements, from the SH0ES and Pantheon+ collaborations, for instance, favor a value of ~73 km\/s\/Mpc, as shown here with smaller error bars. The two sets of values disagree at more than 5-sigma significance.\n<\/p>\n

Credit<\/a>: DESI collaboration, \tarXiv:2404.03002, 2024<\/p>\n

But \u201cearly relic\u201d and \u201cdistance ladder\u201d results for the expansion rate significantly disagree<\/a>.<\/p>\n

\"expansion<\/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 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 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

The early relic method \u2014 tracking baryon acoustic oscillation imprints \u2014 produces 67 km\/s\/Mpc.<\/p>\n

\"acoustic<\/p>\n

We can look arbitrarily far back in the Universe if our telescopes allow, and the clustering of galaxies should reveal a specific distance scale \u2013 the acoustic scale \u2013 that should evolve with time in a particular fashion, just as the acoustic \u201cpeaks and valleys\u201d in the cosmic microwave background reveal this scale as well. The evolution of this scale, over time, is an early relic that reveals a low expansion rate of ~67 km\/s\/Mpc, and is consistent from CMB features to BAO features.\n<\/p>\n

Credit<\/a>: E M Huff, the SDSS-III team and the South Pole Telescope team; graphic by Zosia Rostomian<\/p>\n

Distance ladder methods \u2014 measuring successively more distant objects \u2014 generate 73 km\/s\/Mpc.<\/p>\n

\"Infographic<\/p>\n

The construction of a cosmic distance ladder begins with measuring the parallax of individual stars within the Milky Way and its satellites, such as Cepheids. Then we identify those same stars in nearby galaxies that also house other measurable distance indicators, such as type Ia supernovae, which we then observe at cosmological distances. This allows us to measure the expansion rate of the Universe by starting locally and looking out into the broader Universe.\n<\/p>\n

Credit<\/a>: NASA, ESA, A. Feild (STScI), and A. Riess (STScI\/JHU); Modifications: E. Siegel<\/p>\n

Some argue the distance ladder could be biased<\/a>.<\/p>\n

\"\"<\/p>\n

This graph shows how various selection choices for the sample used in your distance ladder impacts both the average values (data points) and the uncertainties (size of the error bar lines) for a variety of galaxies. Some have JWST data and some have only Hubble data; some have Cepheids and some have asymptotic giant branch stars; some were selected by the CCHP team and some were selected by the SH0ES team, etc. The smallest uncertainties come from studies that use the full suite of data. The Planck data remains with a best-fit estimate of ~67 km\/s\/Mpc.\n<\/p>\n

Credit<\/a>: A.G. Riess et al., Astrophysical Journal submitted, arXiv:2408.11770, 2024<\/p>\n

Could a single bad measurement, or calibration error, explain this tension<\/a> fully?<\/p>\n

\"\"<\/p>\n

This graph of astronomical magnitude (y-axis) versus Cepheid period (x-axis) for Cepheid variable stars in the Large (left) and Small (right) Magellanic Clouds. The stars are shown in two Weisenheit indices (top) and three Hubble filters (bottom) for each one. Once outliers (small x symbols) are excluded, the period-luminosity relations (solid lines) are derived.\n<\/p>\n

Credit<\/a>: L. Breuval et al., Astrophysical Journal submitted\/arXiv:2404.08038, 2024<\/p>\n

To test this, astronomers assembled the Local Distance Network<\/a>.<\/p>\n

\"Diagram<\/p>\n

In this outline of a pipeline to measuring the Hubble constant (the expansion rate of the Universe today), astronomers from the Local Distance Network super-collaboration point out a series of pathways that leverage several independent methods at every step. If all methods converge on the same answer, then no single error in measurement or calibration could be responsible for the tension.\n<\/p>\n

Credit<\/a>: S. Casertano et al., Astronomy & Astrophysics, 2026<\/p>\n

They leveraged many independent measurement techniques<\/a>, testing for any such errors.<\/p>\n

\"\"<\/p>\n

This graphic shows which galaxies that are used as anchors and contain both type Ia supernovae and Cepheids have been imaged by Hubble and JWST, respectively. You can see the change in each galaxy\u2019s contribution to the value of the expansion rate today, H0, by including or excluding each galaxy within the full sample.\n<\/p>\n

Credit<\/a>: A.G. Riess et al., Astrophysical Journal submitted, arXiv:2408.11770, 2024<\/p>\n

Instead of the traditional \u201cparallax \u2192 cepheid \u2192 type Ia supernova\u201d pipeline, many alternatives are considered.<\/p>\n

\"megamaser\"<\/p>\n

This composite Hubble (blue\/white\/dark) and ALMA (red) image shows not only the colliding galaxy system Arp 220, but also the double nucleus which contains the bright emission from both water and hydroxyl megamasers. Astrophysical masers rely on the same underlying physics as lasers, but were actually discovered prior to the 1958 invention of lasers in a laboratory.\n<\/p>\n

Credit<\/a>: ALMA(ESO\/NAOJ\/NRAO)\/NASA\/ESA and The Hubble Heritage Team (STScI\/AURA)<\/p>\n

One can begin with astrophysical masers,<\/p>\n

\"binary<\/p>\n

Binary systems typically have unequal masses, unequal brightnesses, and orbit a barycenter that lies outside of both stars. Only if the alignment with respect to us is sufficiently edge-on, at right, will it appear as an eclipsing binary. Wide binaries, with separations of thousands of astronomical units (AUs), are exceptionally difficult to characterize. Approximately 35% of all stars are found in binary systems, with half in singlet systems and the remainder in trinary or even richer multi-star systems.\n<\/p>\n

Credit<\/a>: Zhatt and Stanlekub\/Wikimedia Commons<\/p>\n

detached eclipsing binaries,<\/p>\n

\"diagram<\/p>\n

In the inner regions of a star that undergoes a core-collapse supernova, a neutron star begins to form in the core, while the outer layers crash against it and undergo their own runaway fusion reactions. Neutrons, neutrinos, radiation, and extraordinary amounts of energy are produced, with neutrinos and antineutrinos carrying the majority of the core-collapse supernova\u2019s energy away. Whether the remnant becomes a neutron star or black hole, ultimately, depends on how much mass remains in the core during this process.\n<\/p>\n

Credit<\/a>: TeraScale Supernova Initiative\/Oak Ridge National Lab<\/p>\n

or type II supernovae,<\/p>\n

\"parallax\"<\/p>\n

The stars that are closest to Earth will appear to shift periodically with respect to the more distant stars as the Earth moves through space in orbit around the Sun. Before the heliocentric model was established, we weren\u2019t looking for \u201cshifts\u201d with a ~300,000,000 kilometer baseline over the span of ~6 months, but rather a ~12,000 kilometer baseline over the span of one night: Earth\u2019s diameter as it rotated on its axis. The distances to the stars are so great that it wasn\u2019t until the 1830s that the first parallax, with a 300 million km baseline, was detected. Today, we\u2019ve measured the parallax of over 1 billion stars with ESA\u2019s Gaia mission.\n<\/p>\n

Credit<\/a>: ESA\/ATG medialab<\/p>\n

not merely parallaxes.<\/p>\n

\"Flowchart<\/p>\n

When the actual data humanity has collected is applied to the various pipeline methods outlined by the Local Distance Network community, a variety of pathways to obtaining the Hubble constant, or the expansion rate today, are obtained. If all the results yield the same answer, then the idea that \u201cone bad measurement\u201d is responsible for the Hubble tension can be ruled out.\n<\/p>\n

Credit<\/a>: S. Casertano et al., Astronomy & Astrophysics, 2026<\/p>\n

One can then progress to Mira variables,<\/p>\n

\"\"<\/p>\n

The star Mira, as shown here as imaged by the GALEX observatory in the ultraviolet, speeds through the interstellar medium at speeds much greater than normal: at about 130 km\/s, which is about ten times faster than typical speeds but is still below the escape velocity of the Milky Way. Mira\u2019s trajectory cannot be traced back to the galactic center, indicating that some lesser gravitational interaction gave it its high-velocity kick. Many stars other than Mira, however, have achieved speeds sufficient to gravitationally unbind them from our home galaxy, with a significant fraction of those being traceable back to the galactic center.\n<\/p>\n

Credit<\/a>: NASA\/JPL-Caltech\/C. Martin (Caltech)\/M. Seibert(OCIW)<\/p>\n

stars at the tip of the red giant branch,<\/p>\n

\"Hertzsprung-Russell<\/p>\n

When stars run out of hydrogen in their cores, they evolve off of the main sequence, becoming subgiants, then red giants, then igniting helium in their cores (which is the tip-of-the-red-giant branch phase), and then evolving onto the horizontal branch and eventually into supergiants (for high-mass stars) or into the asymptotic giant branch (for non-high-mass stars) before dying. The mass of a star determines its ultimate fate, but the rate of fusion is set by other internal properties.\n<\/p>\n

Credit<\/a>: Starhuckster.com<\/p>\n

or asymptotic giant branch stars,<\/p>\n

\"RS<\/p>\n

The Variable Star RS Puppis, with its light echoes shining through the interstellar clouds. Variable stars come in many varieties; one of them, Cepheid variables, can be measured both within our own galaxy and in galaxies up to 50\u201360 million light years away, with all Cepheid variables exhibiting a relationship between their period, or how long it takes them to reach maximum brightness again after fading, and their luminosity, or how intrinsically bright they are.\n<\/p>\n

Credit<\/a>: NASA, ESA, G. Bacon (STScI), the Hubble Heritage Team (STScI\/AURA)-ESA\/Hubble Collaboration, and H. Bond (STScI and Pennsylvania State University)<\/p>\n

not merely Cepheids<\/a>.<\/p>\n

\"Box<\/p>\n

An enormous variety of methods can be used to determine the distance to a host galaxy, several of which are illustrated here: Cepheid and tip of the red giant branch measurements to a variety of galaxies with a variety of telescopes. The uncertainty translates into no more than a 0.04 residual in the distance modulus to any such galaxy, illustrating the smallness of the uncertainty.\n<\/p>\n

Credit<\/a>: S. Casertano et al., Astronomy & Astrophysics, 2026<\/p>\n

And then, one can measure surface brightness fluctuations,<\/p>\n

\"The<\/p>\n

Around galaxy UGC 00180, a great stellar halo consisting of approximately four billion stars\u2019 worth of matter can be discovered by optimizing this telescopic image for low surface-brightness features. When a galaxy is observed with a realistic instrument, its surface brightness will exhibit fluctuations whose magnitude and frequency is dependent not just on the intrinsic properties of the galaxies itself, but also on its distance from us, enabling astronomers to use surface brightness fluctuations to measure cosmic distance.<\/p>\n

Credit<\/a>: Gran Telescopio Canarias (GTC) \/ Gabriel P\u00e9rez (IAC)<\/p>\n

galactic rotation\/velocity dispersion properties,<\/p>\n

\"A<\/p>\n

This animation shows the transition between ESO VISTA data (orange) and ALMA data (blue, white, and red), where the latter shows the velocity profile of what VISTA clearly shows is a disk galaxy. This makes REBELS-25, the galaxy imaged here, the earliest, youngest rotating disk galaxy ever discovered: just 700 million years after the Big Bang.\n<\/p>\n

Credit<\/a>: ALMA (ESO\/NAOJ\/NRAO)\/L. Rowland et al.\/ESO\/J. Dunlop et al. Ack.: CASU, CALET; Animation: E. Siegel<\/p>\n

or type II supernovae,<\/p>\n

\"Cassiopeia<\/p>\n

Back sometime between 1667 and 1680, a core-collapse supernova occurred in the constellation of Cassiopeia, between 9000 and 11000 light-years away. First detected in 1947 in radio light, this VLA image maps out the radio emission coming from this supernova remnant.\n<\/p>\n

Credit<\/a>: Credit: L. Rudnick, T. Delaney, J. Keohane & B. Koralesky, image composite by T. Rector<\/p>\n

not exclusively type Ia supernovae<\/a>.<\/p>\n

\"An<\/p>\n

The beautiful barred spiral galaxy NGC 1015, shown here as imaged by the Hubble Space Telescope in 2013, also contains many Cepheid variable stars as well as an observed, recent Type Ia supernova. This information is used to calibrate the luminosity of the more distant Type Ia supernovae that cannot be measured alongside resolvable Cepheids. A large number of \u201cconnecting\u201d galaxies that have both stellar-type and extragalactic-type indicators in them are needed to solidify the distance ladder.\n<\/p>\n

Credit<\/a>: ESA\/Hubble & NASA, A. Riess (STScl\/JHU)<\/p>\n

The results average to 73.5 km\/s\/Mpc, with just 1.1% uncertainties.<\/p>\n

\"Bar<\/p>\n

Regardless of the direct (distance ladder) method used, the results obtained are all exclusively between 72 and 75 km\/s\/Mpc, with the lone exceptions coming from the CCHP group, whose calibration schemes have been repeatedly questioned and, when independently reanalyzed, brought into alignment with the other results. Note that even though the error bars can be larger with alternative methods, the mean value does not change.\n<\/p>\n

Credit<\/a>: S. Casertano et al., Astronomy & Astrophysics, 2026<\/p>\n

Excluding any one method, indicator, or calibration produces no change.<\/p>\n

\"Bar<\/p>\n

If you insist on the assertion that there\u2019s a single bad method or calibration that\u2019s to blame for the Hubble tension, then the cross-check method of \u201cleaving one out,\u201d whether it\u2019s a distance indicator or a type of measurement method, would reveal a bias in the conclusion. The lack of a meaningful shift in the above analysis is sufficient to rule such a culprit out.\n<\/p>\n

Credit<\/a>: S. Casertano et al., Astronomy & Astrophysics, 2026<\/p>\n

The tension persists<\/a>. \u201cOne bad measurement\u201d cannot be the culprit.<\/p>\n

\"A<\/p>\n

If you measure the expansion rate of the Universe using an early relic method, like the light from the CMB (top right), you get a value of around 67 km\/s\/Mpc. If you measure it by constructing a distance ladder (below left), such as with Cepheids and type Ia supernovae, you get a value more like 73 km\/s\/Mpc. This discrepancy is at the root of the Hubble tension.\n<\/p>\n

Annelisa Leinbach \/ NASA, Adobe Stock<\/p>\n

Mostly Mute Monday tells an astronomical story in images, visuals, and no more than 200 words.<\/p>\n","protected":false},"excerpt":{"rendered":"For 15 years now, the expanding Universe hasn\u2019t added up. This graph shows a comparison between the value…\n","protected":false},"author":2,"featured_media":601369,"comment_status":"","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[23],"tags":[49,48,66,306],"class_list":{"0":"post-601368","1":"post","2":"type-post","3":"status-publish","4":"format-standard","5":"has-post-thumbnail","7":"category-space","8":"tag-ca","9":"tag-canada","10":"tag-science","11":"tag-space"},"_links":{"self":[{"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/posts\/601368","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/comments?post=601368"}],"version-history":[{"count":0,"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/posts\/601368\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/media\/601369"}],"wp:attachment":[{"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/media?parent=601368"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/categories?post=601368"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.newsbeep.com\/ca\/wp-json\/wp\/v2\/tags?post=601368"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}