Another Straw-person SALSA Simulation Amy Connolly UCLA February 4 th, 2005 Work by A. Connolly, D. Saltzerg and D. Williams
Outline of the Code Instrumented region is (2 km) 3 cube Pick interaction position from (8 km) 3 cube beginning 500 m below the Earth’s surface 1000 dipole-like dual-polarization antennas (10 along each edge) MHz Calculate signal detected at each antenna Require 4 hits, each 6 above RMS noise Each event is weighted for prob. of atten. along ’s path length in Earth, salt Simple earth model (core, mantle, crust) Assume salt atten. length ( » 1/ =600 m at 150MHz
The Askaryan Signal: Electric Field Electric field emitted at interaction: For salt (from personal communication w/ J. Alvarez Muniz in Fall 2003) C=1.10 £ 10 -7, 0 =1300 MHz, » 1.5 Compare to ice (J. Alvarez Muniz, astro-ph/ ) C=2.53 £ 10 -7, 0 =1150 MHz, =1.44
The Askaryan Signal: Cone Width Width of Cerenkov cone (astro- ph/ , astro-ph/ , Phys.Lett.B434,396 (1998)): Material dependence Index of refraction Shower length
The Signal: Cone Width (cont) Phys.Lett.B434, 396(1998): Beyond parameterization (>7), scaling by 7.5% per decade. n-dependence? Need theorists to come up with concise instructions for simulating the Askaryan signal, complete for all relevant media
Zenith Angle SALSA only sensitive to down-going ’s distribution independent of energy Cross-section measurement seems difficult
Interaction Position For E =10 19 eV, where events occur that are triggered: Vertical PlaneHorizontal Plane
Sensitivity
Conclusions Simple simulation program written with results similar to Peter’s How high a frequency do we need to go to Need unified message from theorists on simulation of signal
Backup Slides
Trigger Rates 4-fold, 6 ! coincidence rate essentially zero. 4-fold, 4 ! <~ 1/year E =10 18 eV Local coincidence: 20 ns Global coincidence: 10 s