Sterile Neutrinos in July 2010

Similar documents
Carlo Giunti. CERN Particle and Astro-Particle Physics Seminar. work in collaboration with Mario Acero Marco Laveder Walter Winter

Status of Light Sterile Neutrinos Carlo Giunti

Status of Light Sterile Neutrinos Carlo Giunti

Sterile Neutrinos. Carlo Giunti

Status of Sterile Neutrinos Carlo Giunti

Sterile neutrino oscillations

Analysis of Neutrino Oscillation experiments

Two hot issues in neutrino physics

Oscillations Beyond Three-Neutrino Mixing (Status of Light Sterile Neutrinos) Carlo Giunti

Hint of CPT Violation in Short-Baseline Electron Neutrino Disappearance

Impact of light sterile!s in LBL experiments "

Sterile neutrinos. Stéphane Lavignac (IPhT Saclay)

Sterile Neutrino Searches: Experiment and Theory Carlo Giunti INFN, Sezione di Torino

Neutrino Experiments: Lecture 2 M. Shaevitz Columbia University

SNOW Global fits to neutrino oscillation data. Thomas Schwetz SISSA, Trieste

Neutrino Oscillation Measurements, Past and Present. Art McDonald Queen s University And SNOLAB

Unbound Neutrino Roadmaps. MARCO LAVEDER Università di Padova e INFN NOW September 2006

C. Giunti Sterile Neutrino Mixing NOW Sep /25

Phenomenological Status of Neutrino Mixing

Neutrino Masses in Cosmology, Neutrinoless Double-Beta Decay and Direct Neutrino Masses Carlo Giunti

Oscillations Beyond Three-Neutrino Mixing. Carlo Giunti

Short-Baseline Neutrino Oscillation Anomalies and Light Sterile Neutrinos. Carlo Giunti

Updated three-neutrino oscillation parameters from global fits

Stefano Gariazzo. Light sterile neutrino: the 2018 status. IFIC, Valencia (ES) CSIC Universitat de Valencia

Status of the Sterile Neutrino(s) Carlo Giunti

MiniBooNE, LSND, and Future Very-Short Baseline Experiments

Neutrino Physics: Lecture 12

Neutrino Basics. m 2 [ev 2 ] tan 2 θ. Reference: The Standard Model and Beyond, CRC Press. Paul Langacker (IAS) LSND 90/99% SuperK 90/99% MINOS K2K

The reactor antineutrino anomaly & experimental status of anomalies beyond 3 flavors

Status and prospects of neutrino oscillations

Sensitivity to sterile ν mixings at a ν Factory --Side business of a ν Factory --

On Minimal Models with Light Sterile Neutrinos


Neutrino Physics II. Neutrino Phenomenology. Arcadi Santamaria. TAE 2014, Benasque, September 19, IFIC/Univ. València

NEUTRINOS II The Sequel

Sterile neutrinos: to be or not to be?

NEUTRINO OSCILLATIONS AND STERILE NEUTRINO C. Giunti

Recent Discoveries in Neutrino Oscillation Physics & Prospects for the Future

Reactor anomaly and searches of sterile neutrinos in experiments at very short baseline

Neutrino Anomalies & CEνNS

Neutrino Oscillations

Neutrino Oscillations

Neutrinos in Supernova Evolution and Nucleosynthesis

The Reactor Antineutrino Anomaly

Overview of Reactor Neutrino

Neutrinos: Three-Flavor Effects in Sparse and Dense Matter

Neutrino Physics. Carlo Giunti

The future of neutrino physics (at accelerators)

Solar and atmospheric ν s

Particle Physics: Neutrinos part II

Neutrino oscillation experiments: Recent results and implications

How many neutrino species are there?

Updating the Status of Neutrino Physics

Long baseline experiments

Neutrinos. Thanks to Ian Blockland and Randy Sobie for these slides. spin particle with no electric charge; weak isospin partners of charged leptons

1. Neutrino Oscillations

Searching for Physics Beyond the Standard Model with Accelerator ν Experiments W.C Louis, LANL. MiniBooNE Status FNAL ORNL

Search for sterile neutrino mixing in the muon neutrino to tau neutrino appearance channel with the OPERA detector

NEUTRINO AND CPT THEOREM

Critical Review on Neutrino Anomalies. Carlo Giunti

Neutrino Oscillations And Sterile Neutrinos

Neutrinos, Oscillations and New Physics: An Introduction

On indications for sterile neutrinos at the ev scale. Invisibles 14 workshop, July 2014, Paris Thomas Schwetz

Neutrino Mass: Overview of ββ 0ν, Cosmology and Direct Measurements Carlo Giunti

Exotic Charges, Multicomponent Dark Matter and Light Sterile Neutrinos

Dark Radiation and Inflationary Freedom

Solar Neutrino Road Map. Carlos Pena Garay IAS

1 Neutrinos. 1.1 Introduction

ev-scale Sterile Neutrinos

Sterile neutrinos at future long-baseline experiments

Neutrino properties: nature, mass & CP violation

Neutrino mixing II. Can ν e ν µ ν τ? If this happens:

Neutrinos: status, models, string theory expectations

Grand Unification Theories

Ruling out four-neutrino oscillation interpretations of the LSND anomaly?

Neutrino physics. Evgeny Akhmedov. Max-Planck-Institut für Kernphysik, Heidelberg & Kurchatov Institute, Moscow

Introduction to Neutrino Physics

Neutrinos and Cosmos. Hitoshi Murayama (Berkeley) Texas Conference at Stanford Dec 17, 2004

Review of Neutrino Oscillation Experiments

Neutrinos as a Unique Probe: cm

Stefano Gariazzo. Light sterile neutrinos with pseudoscalar interactions in cosmology. Based on [JCAP 08 (2016) 067] University and INFN, Torino

GLOBAL ANALYSIS OF NEUTRINO DATA

The Short Baseline Neutrino Program at Fermilab

Jarek Nowak University of Minnesota. High Energy seminar, University of Virginia

MINOS Result. The ND analysis predicts: events in the Far Detector 54 observed, 0.7σ excess. 49.1±7.0(stat.)±2.7(syst.

Neutrino Oscillations

What We Know, and What We Would Like To Find Out. Boris Kayser Minnesota October 23,

Solar Neutrinos & MSW Effect. Pouya Bakhti General Seminar Course Nov IPM

arxiv: v1 [hep-ex] 22 Jan 2009

Overview of cosmological constraints on neutrino mass, number, and types

Neutrino oscillation phenomenology

Latest Results from MINOS and MINOS+ Will Flanagan University of Texas on behalf of the MINOS+ Collaboration

Future prospects of neutrino oscillation study Osamu Yasuda Tokyo Metropolitan University April 27, IPMU

Neutrino Experiments: Lecture 3 M. Shaevitz Columbia University

The Hunt for Sterile Neutrinos. H. Ray, University of Florida

Neutrino Oscillation Physics

eutrino oscillations - Wikipedia, the free encyclopedia

Searching for Physics Beyond Standard Model with Neutrinos. R.G. Van de Water Los Alamos National Laboratory

How large is the "LSND anomaly"?

Searching for Sterile Neutrinos with an Isotope β-decay Source: The IsoDAR Experiment

Transcription:

Sterile Neutrinos in July 0 Carlo Giunti INFN, Sezione di Torino Presidenza INFN, Roma, 19 July 0 Collaboration with Marco Laveder (Padova University) C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 1

Standard Model: Massless Neutrinos Standard Model: L c R =µ no Dirac mass term Ä D = m D ( L R + R L ) Majorana Neutrino: c = c R = R =µ Majorana mass term Ä M = 1 mm L R c + c R L Standard Model: Majorana mass term not allowed by SU() L U(1) Y (no Higgs triplet) C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0

Neutrinos are special in the Standard Model: the only neutral fermions In extensions of SM neutrinos can mix with non-sm fermions L «L = «L Φ = i Φ = 0 Ô Symmetry v «L Breaking 0 («= e ) L «L Φ can be coupled to new non-sm chiral fermion fields f R Dirac mass terms L «L Φf R + Majorana mass terms f C R f R f R are often called Right-Handed Neutrinos: f R R If f R are light, they are called Sterile Neutrinos: s L = f C R C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 3

Sterile Neutrinos Sterile means No Standard Model Interactions Obviously no electromagnetic interactions as normal active neutrinos Thus Sterile means No Standard Weak Interactions But Sterile Neutrinos are not absolutely sterile: Gravitational Interactions New Non-Standard Interactions of the Physics Beyond the Standard Model which generates the masses of sterile neutrinos Extremely interesting and powerful window on Physics Beyond the SM Active Neutrinos ( e ) can oscillate into Sterile Neutrinos ( s ) Observable: disappearance of Active Neutrinos or indirect evidence through combined fit of data C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 4

How many Sterile Neutrinos? e + e Z µ e 3 active flavor neutrinos mixing µ «L = N k=1 U «k kl «= e N 3 no upper limit! Mass Basis: 1 3 4 5 Flavor Basis: e s1 s ACTIVE STERILE C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 5

Experimental Evidences of Neutrino Oscillations ¼ ½ Homestake Kamiokande Solar GALLEX/GNO & SAGE e Super-Kamiokande msol ³ 7 6 5 ev Reactor e disappearance Atmospheric Accelerator disappearance ¼ SNO BOREXino (KamLAND) Kamiokande IMB Super-Kamiokande MACRO Soudan- (KK & MINOS) ½ sin SOL ³ 0 3 m ATM ³ 4 3 ev sin ATM ³ 0 50 Two scales of m : m ATM ³ 30 m SOL Large mixings: ATM ³ 45 Æ SOL ³ 34 Æ C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 6

Three-Neutrino Mixing «L = 3 k=1 U «k kl («= e ) three flavor fields: e,, three massive fields: 1,, 3 m 1 + m 3 + m 13 = m m 1 +m 3 m +m 1 m 3 = 0 m SOL = m 1 ³ 7 6 5 ev m ATM ³ m 31 ³ m 3 ³ 4 3 ev C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 7

Allowed Three-Neutrino Schemes m m ν 3 ν m SOL ν 1 m ATM m ATM ν m SOL ν 1 ν 3 normal inverted different signs of m 31 ³ m 3 absolute scale is not determined by neutrino oscillation data C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 8

Interesting possibility: a new msbl 1eV It has been studied in connection with searches of neutrino oscillations in Short-BaseLine Experiments L E 1 m MeV =µ m SBL 1eV Necessary introduction of at least one new massive neutrino: 4- Mixing m SBL = m 41 C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 9

Four-Neutrino Schemes: + and 3+1 m m ν 4 ν 4 ν 3 m SBL m SBL ν 3 ν ν + ν 1 3+1 ν 1 C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0

LSND [PRL 75 (1995) 650; PRC 54 (1996) 685; PRL 77 (1996) 308; PRD 64 (001) 11007] e L ³ 30m 0MeV E 00MeV Beam Excess 17.5 15 1.5 7.5 5.5 Beam Excess p(ν _ µ ν_ e,e+ )n p(ν _ e,e+ )n other 1-1 0 0.4 0.6 0.8 1 1. 1.4 - L/E ν (meters/mev) m (ev /c 4 ) Karmen Bugey 90% (L max -L <.3) 99% (L max -L < 4.6) CCFR NOMAD -3 - -1 1 sin θ m LSND 0 ev ( m ATM m SOL ) C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 11

+ Four-Neutrino Schemes m m ν 4 ν m ATM ν 3 m SOL ν 1 m SBL m SBL ν m SOL ν 1 normal ν 4 m ATM ν 3 inverted C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 1

+ Schemes are strongly disfavored by solar and atmospheric data 50 χ 40 30 0 solar + KamLAND solar solar (pre SNO salt) global solar + KamLAND χ PG χ PC 99% CL (1 dof) atm + KK + SBL 0 0 0. 0.4 0.6 0.8 0. 0.4 0.6 0.8 1 η s η s s = U s1 + U s [Maltoni, Schwetz, Tortola, Valle, New J. Phys. 6 (004) 1, arxiv:hep-ph/040517] 99% CL: s 0 5 (solar + KamLAND) s 0 75 (atmospheric + KK) C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 13

3+1 Four-Neutrino Schemes m m m m ν ν 4 ν 4 ν 3 m SOL m ATM ν m ATM ν 1 m SOL ν 1 ν 3 m SBL m SBL m SBL m SBL ν 3 ν m SOL m ATM ν m ATM ν 1 m SOL ν 4 ν 4 ν 1 ν 3 normal 3 -inverted 4 -inverted fully-inverted Perturbation of 3- Mixing U e4 1 U 4 1 U 4 1 U s4 ³ 1 C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 14

Effective SBL Oscillation Probability in 3+1 Schemes P «= sin «sin m L 4E sin «= 4 U «4 U 4 («= ) No CP Violation! P ««= 1 sin ««sin m L 4E sin ««= 4 U «4 1 U «4 U e1 U e U e3 U e4 sin ««1 U = U µ1 U τ1 U µ U τ U µ3 U τ3 U µ4 U τ4 U s1 U s U s3 U s4 SBL U «4 ³ sin ««4 C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 15

e disappearance experiments: sin ee = 4 U e4 1 U e4 ³ 4 U e4 disappearance experiments: sin = 4 U 4 1 U 4 ³ 4 U 4 e experiments: sin e = 4 U e4 U 4 ³ 1 4 sin ee sin Upper bounds on sin ee and sin imply strong limit on sin e C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 16

e Disappearance [Savannah River (SRP), PRD 53 (1996) 6054] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 17

( ) Disappearance [CCFR, Z. Phys. C 7 (1985) 53] [CDHSW, PLB 134 (1984) 81] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 18

99% CL ( ) ( ) e 1 NEV + atm + KK NEV + atm(1d) m LSND [ev ] 0 LSND global LSND DAR -1 95% CL -4-3 - -1 0 sin θ LSND [Maltoni, Schwetz, Tortola, Valle, New J. Phys. 6 (004) 1, arxiv:hep-ph/040517] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 19

MiniBooNE Neutrinos [PRL 98 (007) 31801] e L ³ 541m 475MeV E 3GeV Events / MeV 3.5 1.5 1 Data ν e from µ + ν e from K 0 ν e from K π 0 misid Nγ dirt other Total Background 0.5 0. 0.4 0.6 0.8 1 1. 1.4 1.5 1.6 3. QE E ν (GeV) Excess Events / MeV 0.8 data - expected background best-fit ν µ ν e 0.6 sin θ=0.004, m =1.0eV 0.4 sin θ=0., m =0.1eV 0. 0-0. 0. 0.4 0.6 0.8 1 1. 1.4 1.6 1.5 3. QE E ν (GeV) [PRL (009) 180, arxiv:081.43] Low-Energy Anomaly! [arxiv:0901.1648] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 0

MiniBooNE Antineutrinos [arxiv:07.1150] e L ³ 541m 475MeV E 3GeV Events/MeV 0.6 +/- ν e & ν e from µ Fit Region +/- ν e & ν e from K 0 ν e & ν e from K 0 π misid 0.4 Nγ dirt Events/MeV 0. 0.3 0. other Constr. Syst. Error Best Fit (E>475MeV) Data - expected background Best Fit sin θ=0.004, m =1.0eV ) 4 /c (ev m 1 68% CL 90% CL 99% CL KARMEN 90% CL BUGEY 90% CL 0.1 0.0 sin θ=0.03, m =0.3eV -1 LSND 90% CL -0.1 0. 0.4 0.6 0.8 1.0 1. 1.4 1.5 1.6 3.0 QE E ν (GeV) - -3 LSND 99% CL Agreement with LSND e signal! - sin (θ) Similar L E but different L and E =µ Oscillations! C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 1-1 1

68% CL 90% CL 1 NEV + atm + KK NEV + atm(1d) 99% CL KARMEN 90% CL BUGEY 90% CL m LSND [ev ] 0 LSND global LSND DAR ) 4 /c (ev m 1-1 95% CL 99% CL -4-3 - -1 0-1 LSND 90% CL LSND 99% CL sin θ LSND - -3 - sin (θ) -1 1 Most of LSND and MiniBooNE e allowed region excluded by MiniBooNE e Tension between LSND and MiniBooNE e appearance and e (Bugey) + ( ) (CDHSW+CCFR) disappearance limits Marginally preferred: msbl ³ 0 9eV sin e ³ 3 C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0

Õ m 1 m m 3 m 4 =µ m 4 ³ m41 = m SBL m SBL ³ 0 9eV =µ m 4 ³ 0 9eV Marginally allowed by cosmological limit in ΛCDM (thermalized s s) [Hamann, Hannestad, Raffelt, Tamborra, Wong, arxiv:06.576] Note preference for N s 0 indicated also by BBN C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 3

The primordial abundance of 4 He: evidence for non-standard BBN [Izotov, Thuan, Astrophysical Journal Letters 7 (0) L67, arxiv:01.4440] N = 3 68 +0 80 0 70 N = 3 80 +0 80 0 70 ( ) C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 4

3+ Five-Neutrino Mixing? [Georgia Karagiorgi, Neutrino 0, 14 June 0] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 5

CPT Violation? Masses and mixing of neutrinos and antineutrinos may be different 68% CL 90% CL 99% CL KARMEN 90% CL BUGEY 90% CL In CDHSW mainly s ) 4 /c No limit on SBL e transitions from disappearance experiments [Barger, Marfatia, Whisnant, PLB 576 (003) 303] LSND and MiniBooNE allowed regions are limited only by KARMEN and Bugey (ev m 1-1 - -3 LSND 90% CL LSND 99% CL - sin (θ) -1 1 C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 6

Gallium Anomaly Gallium Radioactive Source Experiments Tests of the solar neutrino detectors GALLEX (Cr1, Cr) and SAGE (Cr, Ar) Detection Process: e + 71 Ga 71 Ge+e e Sources: e + 51 Cr 51 V+ e e + 37 Ar 37 Cl+ e 37Ar (35.04 days) 37Cl (stable) 813 kev ν ( 9.8%) 811 kev ν (90.%) [SAGE, PRC 73 (006) 045805, nucl-ex/051041] [SAGE, PRC 59 (1999) 46, hep-ph/9803418] R Ga = 0 76 +0 09 0 08 [Giunti, Laveder, arxiv:06.344] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 7

Re + 3 H 68.7% C.L. (1σ) 95.45% C.L. (σ) 99.73% C.L. (3σ) m [ev ] + m [ev ] + 1 1 Gallium 68.7% C.L. (1σ) 95.45% C.L. (σ) 99.73% C.L. (3σ) 1 1 sin ϑ [Giunti, Laveder, arxiv:06.344] 1 3 1 sin ϑ [Giunti, Laveder, arxiv:05.4599] m SBL ³ 0 9eV sin sin is OK CPT violation? C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 8

MINOS Hint of CPT Violation LBL disappearance E 3GeV Near Detector at 1.04 km Far Detector at 734 km [MINOS, Neutrino 0, 14 June 0] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 9

Conclusions Existence of sterile neutrinos is possible and likely connected with neutrino mass generation Impressive LSND and MiniBooNE agreement on e signal Three experimental tensions: LSND and MiniBooNE e vs MiniBooNE e LSND and MiniBooNE e vs e and ( ) disappearance limits Gallium Anomaly ( e disappearance) vs Bugey ( e disappearance) Interpretation of experimental results is difficult: 3+1 Four-Neutrino Mixing or more? CPT violation?...? ΛCDM cosmology and BBN indicate N s 0 New experiments are needed! C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 30

MiniBooNE Low-Energy Anomaly Events / MeV 3.5 1.5 1 Data ν e from µ + ν e from K 0 ν e from K π 0 misid Nγ dirt other Total Background 0.5 0. 0.4 0.6 0.8 1 1. 1.4 1.5 1.6 3. [PRL (009) 180, arxiv:081.43] Our Hypothesis: N the j = f P e en cal e j +N cal j QE E ν [Giunti, Laveder, PRD 77 (008) 09300, arxiv:0707.4593; PRD 80 (009) 013005, arxiv:090.199] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 31 (GeV)

N j the = f P e en cal e j +Ncal j Estimated 15% uncertainty of the calculated neutrino flux [MiniBooNE, PRD 79 (009) 0700, arxiv:0806.1449] is consistent with measured ratio 1 1 0 4 of detected and predicted charged-current quasi-elastic events [MiniBooNE, PRL 0 (008) 03301, arxiv:0706.096] We fit MiniBooNE e and data using the info at http://www-boone.fnal.gov/for_physicists/data_release/lowe/ C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 3

events / MeV 0.0 0.5 1.0 1.5.0.5 00 400 600 800 00 100 1400 3000 E [MeV] MiniBooNE ν e N νe,the (j) νe,cal νe,j = f ν P νe νe N νe,j νµ,the νµ,cal N νe,j = f ν N νe,j N the νe,j = N νe,the νµ,the νe,j + N νe,j (b) No Osc. & f = 1 min = 14 3+5 4 NdF = 3+16 GoF = 41% Our Hypothesis min = 0+7 6 NdF = 16 GoF = 89% f = 1 6 sin = 0 3 m = 1 84eV [Giunti, Laveder, 0, arxiv:05.4599] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 33

Note similar best-fit values of sin and m Gallium best fit: sin = 0 7 and m = 09eV MiniBooNE best fit: sin = 0 3 and m = 1 84eV Parameter Goodness of Fit of combined analysis: min = 0 14 NDF = GoF = 93% C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 34

MiniBooNE + Gallium m [ev ] χ 0 4 6 8 1 MB + Ga 68.7% C.L. (1σ) 95.45% C.L. (σ) 99.73% C.L. (3σ) min = 3+9 NdF = 0 GoF = 93% sin = 0 7 + m = 1 9eV 1 1 0 4 6 8 sin ϑ χ [Giunti, Laveder, 0, arxiv:05.4599] C. Giunti Sterile Neutrinos in July 0 Presidenza INFN, Roma, 19 July 0 35