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Euclid preparation. LXXXIX. Accurate and precise data-driven angular power spectrum covariances

This paper introduces DICES, a data-driven method that combines adaptive jackknife resampling with shrinkage toward Gaussian predictions and bias correction to generate accurate, non-singular, and unbiased internal covariances for Euclid's angular power spectrum measurements without relying on cosmological assumptions.

Original authors: Euclid Collaboration, K. Naidoo, J. Ruiz-Zapatero, N. Tessore, B. Joachimi, A. Loureiro, N. Aghanim, B. Altieri, A. Amara, L. Amendola, S. Andreon, N. Auricchio, C. Baccigalupi, D. Bagot, M. Baldi, S.
Published 2026-04-14
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Original authors: Euclid Collaboration, K. Naidoo, J. Ruiz-Zapatero, N. Tessore, B. Joachimi, A. Loureiro, N. Aghanim, B. Altieri, A. Amara, L. Amendola, S. Andreon, N. Auricchio, C. Baccigalupi, D. Bagot, M. Baldi, S. Bardelli, P. Battaglia, A. Biviano, E. Branchini, M. Brescia, S. Camera, V. Capobianco, C. Carbone, V. F. Cardone, J. Carretero, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, A. Da Silva, H. Degaudenzi, G. De Lucia, F. Dubath, X. Dupac, S. Dusini, S. Escoffier, M. Farina, R. Farinelli, S. Farrens, F. Faustini, S. Ferriol, F. Finelli, P. Fosalba, M. Frailis, E. Franceschi, M. Fumana, S. Galeotta, K. George, B. Gillis, C. Giocoli, J. Gracia-Carpio, A. Grazian, F. Grupp, W. Holmes, F. Hormuth, A. Hornstrup, K. Jahnke, M. Jhabvala, E. Keihänen, S. Kermiche, A. Kiessling, M. Kilbinger, B. Kubik, M. Kümmel, M. Kunz, H. Kurki-Suonio, A. M. C. Le Brun, S. Ligori, P. B. Lilje, V. Lindholm, I. Lloro, G. Mainetti, D. Maino, E. Maiorano, O. Mansutti, S. Marcin, O. Marggraf, M. Martinelli, N. Martinet, F. Marulli, R. Massey, E. Medinaceli, S. Mei, Y. Mellier, M. Meneghetti, E. Merlin, G. Meylan, A. Mora, L. Moscardini, C. Neissner, S. -M. Niemi, C. Padilla, S. Paltani, F. Pasian, K. Pedersen, W. J. Percival, V. Pettorino, S. Pires, G. Polenta, M. Poncet, L. A. Popa, F. Raison, R. Rebolo, A. Renzi, J. Rhodes, G. Riccio, E. Romelli, M. Roncarelli, C. Rosset, R. Saglia, Z. Sakr, A. G. Sánchez, D. Sapone, B. Sartoris, P. Schneider, T. Schrabback, A. Secroun, E. Sefusatti, G. Seidel, M. Seiffert, S. Serrano, P. Simon, C. Sirignano, G. Sirri, A. Spurio Mancini, L. Stanco, J. Steinwagner, P. Tallada-Crespí, D. Tavagnacco, A. N. Taylor, I. Tereno, S. Toft, R. Toledo-Moreo, F. Torradeflot, I. Tutusaus, L. Valenziano, J. Valiviita, T. Vassallo, G. Verdoes Kleijn, A. Veropalumbo, Y. Wang, J. Weller, G. Zamorani, F. M. Zerbi, E. Zucca, V. Allevato, M. Ballardini, M. Bolzonella, E. Bozzo, C. Burigana, R. Cabanac, M. Calabrese, A. Cappi, D. Di Ferdinando, J. A. Escartin Vigo, L. Gabarra, J. Martín-Fleitas, S. Matthew, N. Mauri, R. B. Metcalf, A. Pezzotta, M. Pöntinen, I. Risso, V. Scottez, M. Sereno, M. Tenti, M. Viel, M. Wiesmann, Y. Akrami, I. T. Andika, S. Anselmi, M. Archidiacono, F. Atrio-Barandela, A. Balaguera-Antolinez, D. Bertacca, M. Bethermin, A. Blanchard, L. Blot, S. Borgani, M. L. Brown, S. Bruton, A. Calabro, B. Camacho Quevedo, F. Caro, C. S. Carvalho, T. Castro, F. Cogato, S. Conseil, A. R. Cooray, S. Davini, G. Desprez, A. Díaz-Sánchez, J. J. Diaz, S. Di Domizio, J. M. Diego, P. Dimauro, A. Enia, Y. Fang, A. G. Ferrari, P. G. Ferreira, A. Finoguenov, A. Fontana, A. Franco, K. Ganga, J. García-Bellido, T. Gasparetto, V. Gautard, E. Gaztanaga, F. Giacomini, F. Gianotti, G. Gozaliasl, M. Guidi, C. M. Gutierrez, A. Hall, C. Hernández-Monteagudo, H. Hildebrandt, J. Hjorth, S. Joudaki, J. J. E. Kajava, Y. Kang, V. Kansal, D. Karagiannis, K. Kiiveri, C. C. Kirkpatrick, S. Kruk, M. Lattanzi, L. Legrand, M. Lembo, F. Lepori, G. Leroy, G. F. Lesci, J. Lesgourgues, L. Leuzzi, T. I. Liaudat, J. Macias-Perez, G. Maggio, M. Magliocchetti, F. Mannucci, R. Maoli, C. J. A. P. Martins, L. Maurin, M. Miluzio, P. Monaco, C. Moretti, G. Morgante, S. Nadathur, A. Navarro-Alsina, L. Pagano, F. Passalacqua, K. Paterson, L. Patrizii, A. Pisani, D. Potter, S. Quai, M. Radovich, P. -F. Rocci, S. Sacquegna, M. Sahlén, D. B. Sanders, E. Sarpa, A. Schneider, D. Sciotti, E. Sellentin, L. C. Smith, K. Tanidis, G. Testera, R. Teyssier, S. Tosi, A. Troja, M. Tucci, C. Valieri, A. Venhola, D. Vergani, G. Verza, P. Vielzeuf, N. A. Walton

Original paper licensed under CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer

The Big Picture: Mapping the Universe's Invisible Web

Imagine the Euclid Space Telescope as a giant, super-powerful camera sent to take a panoramic photo of the universe. Its goal is to map billions of galaxies to understand Dark Energy (the mysterious force pushing the universe apart) and Dark Matter.

To do this, scientists don't just look at where galaxies are; they look at how they are clustered together and how their shapes are slightly distorted by gravity (a phenomenon called weak lensing). They turn this data into a giant list of numbers called an Angular Power Spectrum.

The Problem:
To trust these numbers, scientists need to know how "noisy" or "uncertain" they are. In statistics, this uncertainty is called a Covariance Matrix. Think of this matrix as a massive spreadsheet that tells you: "If the measurement for Galaxy Group A is a little high, how likely is it that Galaxy Group B is also a little high?"

For the Euclid mission, this spreadsheet is huge (about 100,000 numbers long). The problem is that calculating this spreadsheet accurately is incredibly difficult. If you get it wrong, your entire conclusion about Dark Energy could be wrong.

The Old Way: The "K-Means" Mess

Traditionally, to estimate this uncertainty, scientists use a method called Jackknife Resampling.

  • The Analogy: Imagine you have a giant pizza (the sky). To see how consistent the taste is, you cut the pizza into slices, eat one slice, and taste the rest. Then you put that slice back, eat a different one, and taste the rest again. You repeat this for every slice.
  • The Flaw: The old way of cutting the pizza (using an algorithm called k-means) was messy. Some slices were huge, some were tiny, and some were weird shapes. Because the slices weren't equal, the "taste test" was biased. Also, with a pizza that big, you'd need to cut it into thousands of slices to get a good result, which takes forever to compute.

The New Solution: DICES

The authors of this paper developed a new, smarter way to do this. They call their method DICES (Debiased Internal Covariance Estimation with Shrinkage).

Here is how DICES works, broken down into three simple steps:

1. The Perfect Pizza Cutter (Binary Space Partitioning)

Instead of the messy old cutter, they used a new algorithm called Binary Space Partitioning (BSP).

  • The Analogy: Imagine you have a piece of dough (the survey area on the sky). Instead of guessing where to cut, you take a knife, find the exact center of the dough, and cut it perfectly in half. Then, you take one half, find its center, and cut it in half again. You keep doing this until you have hundreds of tiny, perfectly equal-sized pieces.
  • Why it helps: This ensures every "slice" of the sky is exactly the same size. This removes a major source of error that plagued previous methods. They even made a free app called SkySegmentor so anyone can use this perfect cutter.

2. The "Shrinkage" Trick (Smoothing the Noise)

Even with perfect slices, the data is still "noisy" (like static on an old TV). If you try to calculate the uncertainty matrix directly from this noisy data, the math breaks down (the matrix becomes "singular," meaning it can't be used).

  • The Analogy: Imagine you are trying to draw a map of a coastline based on a sketchy, shaky hand-drawing. The lines are wobbly. To fix it, you take a ruler and gently "shrink" your wobbly lines toward a smooth, theoretical coastline you know exists (a Gaussian prediction). You don't erase your drawing; you just nudge it toward the truth.
  • Why it helps: This "shrinkage" smooths out the random noise, making the math workable and the results stable, without losing the real signal.

3. The "De-Biasing" Correction (Fixing the Over-estimation)

There was one last problem: The old methods tended to overestimate the uncertainty (they thought the data was noisier than it actually was).

  • The Analogy: Imagine you are guessing the weight of a watermelon. The old method was like saying, "It's probably heavy, maybe 20 pounds!" even if it's only 10. The authors realized their "guessing machine" had a built-in error that made everything look heavier.
  • The Fix: They used a clever statistical trick (called a delete-2 jackknife) to measure exactly how much their machine was over-estimating. Then, they subtracted that extra weight.
  • The Result: They combined the "smoothed" map (from step 2) with the "corrected weight" (from step 3).

The Result: A Crystal Clear Map

By combining these three steps, the DICES method produces a covariance matrix that is:

  1. Accurate: It matches the "true" uncertainty much better than before.
  2. Stable: It doesn't break down mathematically, even with huge amounts of data.
  3. Unbiased: It doesn't overestimate the errors.

The Bottom Line:
The Euclid telescope is about to take the most detailed picture of the universe ever made. But a picture is only as good as the frame you put it in. This paper provides the perfect frame. It ensures that when Euclid tells us about Dark Energy, we can trust the numbers completely, because the scientists have figured out exactly how to measure the uncertainty without relying on guesswork.

In short: They invented a better way to cut the sky, a better way to smooth the noise, and a better way to fix the math, ensuring that our understanding of the universe's future is built on solid ground.

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