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1.
Public Health Rep ; 129 Suppl 4: 136-44, 2014.
Article in English | MEDLINE | ID: mdl-25355985

ABSTRACT

OBJECTIVE: We tested the Analytical Hierarchy Process tool for its use in public health to identify potential gaps in emergency preparedness by local health departments (LHDs) in California and Hawaii during a radiological emergency. METHODS: We developed a dedicated tool called All-Hazards Preparedness Squared (AHP2) that can be used by those who are responsible for all-hazards preparedness planning and response to guide them while making strategic decisions both in preparing for and responding to a slow-moving incident while it is unfolding. The tool is an Internet-based survey that can be distributed among teams responsible for emergency preparedness and response. Twenty-eight participants from 16 LHDs in California and Hawaii responsible for coordinating preparedness and response in a radiological emergency participated in using the tool in 2013. We used the data to compare the perceived importance of different elements of preparedness among participants and identify gaps in preparedness of their organizations for meeting the challenges presented by a radiological incident. RESULTS: Clarity of information and transfer of information (to and from agency to public, state, and federal partners) were public health officials' dominant concerns while responding to an emergency. Participants also found that there were gaps in the adequacy of training and awareness of the chain of command during a radiological emergency. CONCLUSION: This preliminary study indicates that the AHP2 tool could be used for decision making in all-hazards preparedness planning and response.


Subject(s)
Disaster Planning/methods , Local Government , Nuclear Warfare , Public Health Administration , Radioactive Hazard Release , Regional Health Planning/methods , California , Civil Defense , Hawaii , Humans , Internet , Surveys and Questionnaires
2.
Phys Rev Lett ; 101(9): 091302, 2008 Aug 29.
Article in English | MEDLINE | ID: mdl-18851600

ABSTRACT

We report the direct measurement of the 7Be solar neutrino signal rate performed with the Borexino detector at the Laboratori Nazionali del Gran Sasso. The interaction rate of the 0.862 MeV 7Be neutrinos is 49+/-3stat+/-4syst counts/(day.100 ton). The hypothesis of no oscillation for 7Be solar neutrinos is inconsistent with our measurement at the 4sigma C.L. Our result is the first direct measurement of the survival probability for solar nu(e) in the transition region between matter-enhanced and vacuum-driven oscillations. The measurement improves the experimental determination of the flux of 7Be, pp, and CNO solar nu(e), and the limit on the effective neutrino magnetic moment using solar neutrinos.

3.
Phys Rev Lett ; 92(18): 181301, 2004 May 07.
Article in English | MEDLINE | ID: mdl-15169480

ABSTRACT

The Sudbury Neutrino Observatory has precisely determined the total active (nu(x)) 8B solar neutrino flux without assumptions about the energy dependence of the nu(e) survival probability. The measurements were made with dissolved NaCl in heavy water to enhance the sensitivity and signature for neutral-current interactions. The flux is found to be 5.21 +/- 0.27(stat)+/-0.38(syst) x 10(6) cm(-2) s(-1), in agreement with previous measurements and standard solar models. A global analysis of these and other solar and reactor neutrino results yields Deltam(2)=7.1(+1.2)(-0.6) x 10(-5) eV(2) and theta=32.5(+2.4)(-2.3) degrees. Maximal mixing is rejected at the equivalent of 5.4 standard deviations.

4.
Phys Rev Lett ; 92(10): 102004, 2004 Mar 12.
Article in English | MEDLINE | ID: mdl-15089201

ABSTRACT

Data from the Sudbury Neutrino Observatory have been used to constrain the lifetime for nucleon decay to "invisible" modes, such as n-->3nu. The analysis was based on a search for gamma rays from the deexcitation of the residual nucleus that would result from the disappearance of either a proton or neutron from 16O. A limit of tau(inv)>2 x 10(29) yr is obtained at 90% confidence for either neutron- or proton-decay modes. This is about an order of magnitude more stringent than previous constraints on invisible proton-decay modes and 400 times more stringent than similar neutron modes.

5.
Phys Rev Lett ; 89(1): 011301, 2002 Jul 01.
Article in English | MEDLINE | ID: mdl-12097025

ABSTRACT

Observations of neutral-current nu interactions on deuterium in the Sudbury Neutrino Observatory are reported. Using the neutral current (NC), elastic scattering, and charged current reactions and assuming the standard 8B shape, the nu(e) component of the 8B solar flux is phis(e) = 1.76(+0.05)(-0.05)(stat)(+0.09)(-0.09)(syst) x 10(6) cm(-2) s(-1) for a kinetic energy threshold of 5 MeV. The non-nu(e) component is phi(mu)(tau) = 3.41(+0.45)(-0.45)(stat)(+0.48)(-0.45)(syst) x 10(6) cm(-2) s(-1), 5.3sigma greater than zero, providing strong evidence for solar nu(e) flavor transformation. The total flux measured with the NC reaction is phi(NC) = 5.09(+0.44)(-0.43)(stat)(+0.46)(-0.43)(syst) x 10(6) cm(-2) s(-1), consistent with solar models.

6.
Phys Rev Lett ; 89(1): 011302, 2002 Jul 01.
Article in English | MEDLINE | ID: mdl-12097026

ABSTRACT

The Sudbury Neutrino Observatory (SNO) has measured day and night solar neutrino energy spectra and rates. For charged current events, assuming an undistorted 8B spectrum, the night minus day rate is 14.0%+/-6.3%(+1.5%)(-1.4%) of the average rate. If the total flux of active neutrinos is additionally constrained to have no asymmetry, the nu(e) asymmetry is found to be 7.0%+/-4.9%(+1.3%)(-1.2%). A global solar neutrino analysis in terms of matter-enhanced oscillations of two active flavors strongly favors the large mixing angle solution.

7.
Phys Rev Lett ; 87(7): 071301, 2001 Aug 13.
Article in English | MEDLINE | ID: mdl-11497878

ABSTRACT

Solar neutrinos from (8)B decay have been detected at the Sudbury Neutrino Observatory via the charged current (CC) reaction on deuterium and the elastic scattering (ES) of electrons. The flux of nu(e)'s is measured by the CC reaction rate to be straight phi(CC)(nu(e)) = 1.75 +/- 0.07(stat)(+0.12)(-0.11)(syst) +/- 0.05(theor) x 10(6) cm(-2) s(-1). Comparison of straight phi(CC)(nu(e)) to the Super-Kamiokande Collaboration's precision value of the flux inferred from the ES reaction yields a 3.3 sigma difference, assuming the systematic uncertainties are normally distributed, providing evidence of an active non- nu(e) component in the solar flux. The total flux of active 8B neutrinos is determined to be 5.44+/-0.99 x 10(6) cm(-2) s(-1).

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