Transcript Document

NO-VE III International Workshop on: "Neutrino Oscillations in Venice" Session:

Tribute to John Bahcall

Solar Neutrinos

Gianluigi Fogli

Outline

John Bahcall: Memories of our interactions Solar

physics: Established facts Solar

physics: Are there little

cracks

?

Conclusions

Based on work with E. Lisi, A. Marrone, A. Palazzo, and A.M. Rotunno Gianluigi Fogli "Neutrino Oscillations in Venice" 2

John Bahcall: Memories of our interactions

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John Bahcall ’ s countless seminars on the solar neutrino problem as a window to new physics are probably responsible for the interest in neutrino physics of many people in this audience - and they were definitely so for myself, in the early 90 ’ s.

[Milla is also responsible in part: My first published contribution to neutrino physics was a talk on “ Problems with Solar Neutrinos ” at her Neutrino Telescope Workshop in 1993 … ]

In collaboration with Eligio Lisi, I then gradually moved from electroweak precision physics to neutrinos. John ’ s book on “ Neutrino Astrophysics ” was the very first guidance in this new (for us) field of physics.

More direct interactions with John started in 1994, with correspondence on his famous Princeton).

“ 1,000 Standard Solar Models ” (that we used to deal with SSM errors and correlations) and with his acceptance of Eligio as an INFN postdoc at his Institution (IAS, Gianluigi Fogli "Neutrino Oscillations in Venice" 4

Interactions with John have been always both scientifically interesting and personally enjoyable.

I remember with great pleasure his participation to the Neutrino Oscillation Workshop in Otranto (NOW 2000), where he managed to come - and to present new results (the preliminary BP 2000 SSM) despite many other obligations he had in that period.

With the same great pleasure I remember his “ laurea honoris causa Committee: ” at Milano in May 2004, with several of us in the Laurea a witness of the close bond of friendship with all of us in Italy.

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These are just facets, from a personal perspective, of his life-long commitment to science, and to the scientific community. Any of us can add countless examples of such commitment. He was really a leading scientist in our field, and we all miss him greatly.

But, his greatest accomplishment remains with us: solar neutrinos as a window to new physics.

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Solar Neutrinos: Some Established Facts

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Fact #1:

Solar  astronomy is an established and recognized branch of science … Sun direction from neutrinos (SK) Earth orbit from solar  (SK) Artist’s view of solar  Gianluigi Fogli (Nobel 2002 - “annus mirabilis”) "Neutrino Oscillations in Venice" 8

Fact #2:

… It requires enduring efforts and difficult experiments … The Pioneers Gianluigi Fogli John ’ s summary of 40 years of expt+theo work "Neutrino Oscillations in Venice" 9

Fact #3:

… But it can be very rewarding in terms of new physics … Each experiment (Cl, Ga, SK, SNO) requires nonzero  mass/mixing Data consistent with each other in terms of mass-mixing parameters All current data converge towards a unique (LMA) solution Gianluigi Fogli "Neutrino Oscillations in Venice" 10

Fact #4:

… Solar  data are also consistent with SSM predictions …  B vs.

Slanted ellipse = model-indep.

combination of SNO-CC, SNO-NC and SK-ES data.

The data overconstrain the two variables … .

… and are consistent with  B from SSM and

< 1 no new solar physics required neutrino flavor change required Gianluigi Fogli "Neutrino Oscillations in Venice" 11

Fact #5:

… and consistent with independent (KamLAND) reactor data … Gianluigi Fogli "Neutrino Oscillations in Venice" 12

Fact #6:

… and consistent with the predicted MSW effects … Study of the tolerance of the solar data for variations of standard MSW interaction energy V = 2 G F N e through a shift V  V · a MSW Case of no matter effects in the Sun is ruled out at >5 sigma.

Clear indication in favor of standard matter effects ( a MSW = 1 ) .

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Fact #7:

… and consistent with small  13 (

… almost competitively with the CHOOZ+SK ATM bound on  13 !

[This and previous plots from GLF, Lisi, Marrone & Palazzo, hep-ph/0506083] Gianluigi Fogli "Neutrino Oscillations in Venice" 15

Fact #8:

Overall agreement is so good that any conceivable “ perturbation ” can be constrained An unorthodox example: Herndon ’ s natural reactor in the Earth ’ s core Solar/KamLAND agreement ruined by neutrino flux from hypothetical georeactor: P GEO < 13 TW at 95% C.L.

Gianluigi Fogli [GLF, Lisi, Palazzo & Rotunno, hep-ph/0505081] "Neutrino Oscillations in Venice" 16

Solar

physics: Are there little

cracks

?

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The previous beautiful and solid facts should not make us exceedingly confident in our current understanding of solar neutrino physics.

Words of caution came from John Bahcall himself: “ Half of all three-sigma results are wrong ” (one of his favorite quotes) “ This is the first time in 40 years of giving talks in solar neutrinos that it seems to me that the people in the audience are more confident of the solar model predictions than I am ” (statement at Neutrino 2002) So we should not be blind to small “ cracks ” , that might open up in the beautiful solar neutrino construction.

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1. SSM predictions and helioseismological data This is one of the possible “ crack late interests of John Bahcall. It occurs when the newest metal abundance estimates are adopted.

” , that has had a central role in the Curiously, such revised metal estimates were motivated by better analyses of the solar atmosphere, rather than by new data.

In this sense: or, in Italian: “ Better is worse ” (John Bahcall, astro-ph/0511337 ) “ Il meglio è nemico del bene ” Gianluigi Fogli "Neutrino Oscillations in Venice" 19

John Bahcall, Physics World, February 2005: “ Chemical controversy at the solar surface ” Fractional difference between measured and predicted values of the speed of sound in the interior of the Sun vs. the solar Radius: Sound speed profile no longer in good agreement with new metallicity (blue curve) Previously, agreement was very good along the whole profile (red curve).

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No clear solution is emerging for the metallicity problem, as also recognized in John ’ s last paper (astro-ph/0511337). There is no “ recommended ” SSM metal input at present.

Luckily, the effect on current solar neutrino mass-mixing parameters is marginal, because: All SSM metal input uncertainties (included and properly propagated in our analysis) are conservatively large; SNO (which dominates solar neutrino fits) measures the below).

8 B flux with an error a factor of ~2 smaller than typical SSM predictions (see figure From Bahcall, Serenelli, Basu astro-ph/0511337: SNO data vs. 10,000 SSM with new metal abundances + optimistic errors ( “ worst case ” for helioseismology) Therefore, all previous mass/mixing bounds are largely insensitive to SSM “ metallicity perturbations ” .

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2. A smaller neutrino-Gallium cross section at low-energy ?

This is another small “ discrepancy ” , which might have some implications on solar neutrino parameter estimation.

The recent claim (Dec. 2005) comes from the combined radioactive source experiments at SAGE & GALLEX/GNO [see the SAGE Collaboration paper, nucl-ex/0512041] Combination (nucl-ex/0512041): measured predicted = 0.88

± 0.05 (1  total error) Gianluigi Fogli where “ predicted ” refers to the Ga cross section calculation by John Bahcall, hep-ph/9710491 "Neutrino Oscillations in Venice" 22

The radioactive “ calibration ” data seem to suggest a downward revision of the low-energy (< 2 MeV) solar neutrino cross-section on Gallium, relevant for the pp, pep, Be, N, and O contributions, by more than 2 sigma (not a negligible shift) The high-energy cross section (> 2 MeV), relevant for the B and hep contributions, is instead basically decoupled from the low-energy one (see John ’ s Gallium cross-section paper, hep-ph/9710491).

Therefore, it is tempting to see what happens if the predicted LE contributions in Ga experiments are renormalized by 0.88

± 0.05

(with HE contributions from 8 B and hep unchanged).

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Our preliminary results for this exercise seem to show that, at face value, such a “ Ga cross section renormalization ” : Worsen the current agreement between Ga and SNO data; Worsen the reliability of the current bounds on only.

 13 from solar  data In order to understand such results, let us recall that the relation between 2  survival probability (  13 =0) and 3  survival probability (  13 >0): and that P  ee changes with energy in the LMA solution: Gianluigi Fogli "Neutrino Oscillations in Venice" 24

Low energy: (small matter effects) High energy: (dominant matter effects) As a consequence: Gianluigi Fogli "Neutrino Oscillations in Venice" 25

In general, to keep the predicted Gallium rate constant (LE): if  13 increases, then  12 must decrease.

Viceversa, to keep the predicted SNO CC/NC ratio constant (HE): if  13 increases, then  12 must increase.

The different behavior of LE and HE rates is at the root of the upper bound on  13 from solar neutrino data only (see S. Goswami and A.Yu. Smirnov, hep-ph/0411359) Gianluigi Fogli "Neutrino Oscillations in Venice" 26

The current situation, without Ga cross-section renormalization, is that: 1) Ga and SNO data (bands) are in very good agreement with predictions (curves) for  13 =0 and sin 2  12 =0.31.

2) The agreement is ruined for increasing  13 , since the Ga and SNO allowed regions drift in different directions of sin 2 other data) places an upper bound on  13  12 ; this fact (together with the from solar neutrino data only.

agreement at  increasing mismatch at  13 13 =0, >0 agreement at  13 =0 Gianluigi Fogli "Neutrino Oscillations in Venice" 27

The situation with Ga cross-section renormalization (0.88

± 0.05 at LE), is that: 1) Ga and SNO data are no longer in good agreement with predictions for (Ga prefers lower sin 2  12 )  13 =0 2) The disagreement becomes rapidly worse for increasing SNO allowed regions become even more separated in sin 2  13 , since the Ga and  12 .

3) Thus, there is never a very good agreement between Ga and SNO constraints, in particular for nonzero  13 .

mismatch at  increasing mismatch at  13 13 =0, >0 mismatch at  13 =0 Gianluigi Fogli "Neutrino Oscillations in Venice" 28

As a consequence, with from “ solar data only ” “ renormalized ” agreement not particularly good even at Ga cross-section, the bound on becomes stronger, but also less reliable (LE-HE  13 =0):  13 Standard Ga cross section “ Renormalized ” Ga cross section Gianluigi Fogli (Recommended bounds) "Neutrino Oscillations in Venice" 29

In conclusion, a smaller Ga cross section (as suggested by the SAGE paper) seems to create a small “ disturbance ” in the current solar neutrino construction. Of course, it ’ s too early to tell if it is an innocent fluctuation or a hint at something deeper.

Certainly, it provides a reason to revisit the theoretical neutrino absorption cross section on Ga and, in general, it provides one more motivation to perform new solar neutrino experiments and solar neutrino spectroscopy in the low-energy range: two topics (among many others) where John ’ s contribution and support will be greatly missed.

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Conclusions

Solar neutrinos provide us with solid evidence for  mass & mixing, and with a beautiful synthesis of physics and astrophysics.

But … as for any synthesis, we are eager to go beyond it! More accurate (astro)physical measurements, or further explorations of the low-energy domain, might reveal something unexpected.

Time will tell us if current section) will grow or die.

“ disturbances ” (metallicity problem, Ga cross A good place to discuss further these and other issues will be

NOW 2006

Conca Specchiulla (Otranto), September 9-16 www.ba.infn.it/ ˜now2006 Gianluigi Fogli "Neutrino Oscillations in Venice" 31