From Wikipedia, the free encyclopedia
Jump to navigation Jump to search

In theoretical physics, fine-tuning is the process in which parameters of a model must be adjusted very precisely in order to fit with certain observations. This had led to the discovery that the fundamental constants and quantities fall into such an extraordinarily precise range that if it did not, the origin and evolution of conscious agents in the universe would not be permitted.[1]

Theories requiring fine-tuning are regarded as problematic in the absence of a known mechanism to explain why the parameters happen to have precisely the observed values that they return. The heuristic rule that parameters in a fundamental physical theory should not be too fine-tuned is called naturalness.[2][3]


The idea that naturalness will explain fine tuning was brought into question by Nima Arkani-Hamed, a theoretical physicist, in his talk "Why is there a Macroscopic Universe?", a lecture from the mini-series "Multiverse & Fine Tuning" from the "Philosophy of Cosmology" project, a University of Oxford and Cambridge Collaboration 2013. In it he describes how naturalness has usually provided a solution to problems in physics; and that it had usually done so earlier than expected. However, in addressing the problem of the cosmological constant, naturalness has failed to provide an explanation though it would have been expected to have done so a long time ago.

The necessity of fine-tuning leads to various problems that do not show that the theories are incorrect, in the sense of falsifying observations, but nevertheless suggest that a piece of the story is missing. For example, the cosmological constant problem (why is the cosmological constant so small?); the hierarchy problem; and the strong CP problem, among others.

Also, Dongshan He's team has suggested a possible solution for the fine tuned Cosmological constant by the universe creation from nothing model.[4]


An example of a fine-tuning problem considered by the scientific community to have a plausible "natural" solution is the cosmological flatness problem, which is solved if inflationary theory is correct: inflation forces the universe to become very flat, answering the question of why the universe is today observed to be flat to such a high degree.[citation needed]


Although fine-tuning was traditionally measured by ad hoc fine-tuning measures, such as the Barbieri-Giudice-Ellis measure, over the past decade many scientists recognized that fine-tuning arguments were a specific application of Bayesian statistics.[5][6][7][8][9][10]

See also[edit]


  1. ^ Leslie, John (1998). Modern Cosmology & Philosophy. University of Michigan: Prometheus Books. ISBN 1573922501.
  2. ^ Grinbaum, Alexei (1 February 2012). "Which Fine-Tuning Arguments Are Fine?". Foundations of Physics. 42 (5): 615–631. arXiv:0903.4055. Bibcode:2012FoPh...42..615G. doi:10.1007/s10701-012-9629-9. S2CID 15590514.
  3. ^ Giudice, Gian (2008). Naturally Speaking: The Naturalness Criterion and Physics at the LHC. Perspectives on LHC Physics. pp. 155–178. arXiv:0801.2562. doi:10.1142/9789812779762_0010. ISBN 978-981-277-975-5. S2CID 15078813.
  4. ^ He, Dongshan; Gao, Dongfeng; Cai, Qing-yu (April 2014). "Spontaneous creation of the universe from nothing". Physical Review. 89 (8): 083510. arXiv:1404.1207. Bibcode:2014PhRvD..89h3510H. doi:10.1103/PhysRevD.89.083510. S2CID 118371273.
  5. ^ Barbieri, R.; Giudice, G.F. (August 1988). "Upper bounds on supersymmetric particle masses". Nuclear Physics B. 306 (1): 63–76. Bibcode:1988NuPhB.306...63B. doi:10.1016/0550-3213(88)90171-X.
  6. ^ Fowlie, Andrew; Balazs, Csaba; White, Graham; Marzola, Luca; Raidal, Martti (17 August 2016). "Naturalness of the relaxion mechanism". Journal of High Energy Physics. 2016 (8): 100. arXiv:1602.03889. Bibcode:2016JHEP...08..100F. doi:10.1007/JHEP08(2016)100. S2CID 119102534.
  7. ^ Fowlie, Andrew (10 July 2014). "CMSSM, naturalness and the ?fine-tuning price? of the Very Large Hadron Collider". Physical Review D. 90 (1): 015010. arXiv:1403.3407. Bibcode:2014PhRvD..90a5010F. doi:10.1103/PhysRevD.90.015010. S2CID 118362634.
  8. ^ Fowlie, Andrew (15 October 2014). "Is the CNMSSM more credible than the CMSSM?". The European Physical Journal C. 74 (10). arXiv:1407.7534. doi:10.1140/epjc/s10052-014-3105-y. S2CID 119304794.
  9. ^ Cabrera, Maria Eugenia; Casas, Alberto; Austri, Roberto Ruiz de (2009). "Bayesian approach and naturalness in MSSM analyses for the LHC". Journal of High Energy Physics. 2009 (3): 075. arXiv:0812.0536. Bibcode:2009JHEP...03..075C. doi:10.1088/1126-6708/2009/03/075. S2CID 18276270.
  10. ^ Fichet, S. (18 December 2012). "Quantified naturalness from Bayesian statistics". Physical Review D. 86 (12): 125029. arXiv:1204.4940. Bibcode:2012PhRvD..86l5029F. doi:10.1103/PhysRevD.86.125029. S2CID 119282331.