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    Mrs. Cary L. Mitchell

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      Mrs. Cary L. Mitchell, new secretary of the Fort Worth Art Center School, looks at a photograph of author Somerset Maugham by Ida Kar. Fort Worth Star-Telegram Morning January 8, 1967.https://mavmatrix.uta.edu/specialcollections_startelegram1960s/3568/thumbnail.jp
      MavMatrix (University of Texas at Arlington)

      The Opinion – Volume 33, No. 1, August 1990

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      Table of Contents Nien Cheng to Kick Off Distinguished Speakers Series / Edie Michalski; Donn McLennen Love in the Law / Wiese/Olson Separate but Better Off? or is One Person, One Vote Still Valid? / Lowell J. Satre Jr. An Era of Strict Construction / Michael J. Varani A Proposal for More Effective Teaching at William Mitchell / Neil W. Hamilton Clinic Curriculum A Gold Mine of Opportunity / Resa Gilats One L; Who is This Cardozo Guy? / Mike Broback An Exclusive Interview with Chief Justice Warren E. Burger Editorial Board Richard J. Olsen (Editor in Chief); Karl Green; M. O\u27Sullivan Kane; Eric Douglas Larson; Tony Schertler; Tamara Tegeler; Robert Christensen; Tom Weiss; Richard K. Ellison; Mike Brobackhttps://open.mitchellhamline.edu/the-opinion/1113/thumbnail.jp
      bepress Legal Repository
      Mitchell Hamline School of Law

      William L. Giles, John K. Bettersworth, E. E. Mitchell, Francis Rhodes, Donations

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        MSU officials William L. Giles, Dr. John K. Bettersworth, E. E. Mitchell, and Dr. Francis Rhodes receive a $1,000 check from the Union Carbide Corporation for the unrestricted use of the Industrial Technology Department.https://scholarsjunction.msstate.edu/ua-photo-collection/3981/thumbnail.jp
        Scholars Junction - Mississippi State University Institutional Repository

        Measurements of K S 0 KS0 {K}_S^0 - K L 0 KL0 {K}_L^0 asymmetries in the decays Λ c + → p K L , S 0 Λc+→pKL,S0 {\Lambda}_c^{+}\to p{K}_{L,S}^0 , p K L , S 0 π + π − pKL,S0π+π− p{K}_{L,S}^0{\pi}^{+}{\pi}^{-} and p K L , S 0 π 0 pKL,S0π0 p{K}_{L,S}^0{\pi}^0

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        Abstract Using e + e − annihilation data sets corresponding to an integrated luminosity of 4.5 fb −1, collected with the BESIII detector at center-of-mass energies between 4.600 and 4.699 GeV, we report the first measurements of the absolute branching fractions B Λ c + → p K L 0 B(Λc+→pKL0) \mathcal{B}\left({\Lambda}_c^{+}\to p{K}_L^0\right) = (1.67 ± 0.06 ± 0.04)%, B Λ c + → p K L 0 π + π − B(Λc+→pKL0π+π−) \mathcal{B}\left({\Lambda}_c^{+}\to p{K}_L^0{\pi}^{+}{\pi}^{-}\right) = (1.69 ± 0.10 ± 0.05)%, and B Λ c + → p K L 0 π 0 B(Λc+→pKL0π0) \mathcal{B}\left({\Lambda}_c^{+}\to p{K}_L^0{\pi}^0\right) = (2.02 ± 0.13 ± 0.05)%, where the first uncertainties are statistical and the second systematic. Combining with the known branching fractions of Λ c + → p K S 0 Λc+→pKS0 {\Lambda}_c^{+}\to p{K}_S^0 , Λ c + → p K S 0 π + π − Λc+→pKS0π+π− {\Lambda}_c^{+}\to p{K}_S^0{\pi}^{+}{\pi}^{-} , and Λ c + → p K S 0 π 0 Λc+→pKS0π0 {\Lambda}_c^{+}\to p{K}_S^0{\pi}^0 , we present the first measurements of the K S 0 KS0 {K}_S^0 - K L 0 KL0 {K}_L^0 asymmetries R Λ c + K S , L 0 X = B Λ c + → K S 0 X − B Λ c + → K L 0 X B Λ c + → K S 0 X + B Λ c + → K L 0 X R(Λc+,KS,L0X)=B(Λc+→KS0X)−B(Λc+→KL0X)B(Λc+→KS0X)+B(Λc+→KL0X) R\left({\Lambda}_c^{+},{K}_{S,L}^0X\right)=\frac{\mathcal{B}\left({\Lambda}_c^{+}\to {K}_S^0X\right)-\mathcal{B}\left({\Lambda}_c^{+}\to {K}_L^0X\right)}{\mathcal{B}\left({\Lambda}_c^{+}\to {K}_S^0X\right)+\mathcal{B}\left({\Lambda}_c^{+}\to {K}_L^0X\right)} in charmed baryon decays: R Λ c + p K S , L 0 = − 0.025 ± 0.031 R(Λc+,pKS,L0)=−0.025±0.031 R\left({\Lambda}_c^{+},p{K}_{S,L}^0\right)=-0.025\pm 0.031 , R Λ c + p K S , L 0 π + π − = − 0.027 ± 0.048 R(Λc+,pKS,L0π+π−)=−0.027±0.048 R\left({\Lambda}_c^{+},p{K}_{S,L}^0{\pi}^{+}{\pi}^{-}\right)=-0.027\pm 0.048 and R Λ c + p K S , L 0 π 0 = − 0.015 ± 0.046 R(Λc+,pKS,L0π0)=−0.015±0.046 R\left({\Lambda}_c^{+},p{K}_{S,L}^0{\pi}^0\right)=-0.015\pm 0.046 . No significant asymmetries with statistical significance are observed
        Infoscience - École polytechnique fédérale de Lausanne
        Directory of Open Access Journals
        Archivio istituzionale della ricerca - Università di Ferrara
        GSI Repository

        Oh, if you went to go a - s p a r k i n ' , I ' l l t e l l you where to go,

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        voiceCollected by Merlin Mitchell Transcribed by Kyle Ferrin Mary Briscoe High, Ark. April 15, 1950 Reel 34 Item 4 I f You Want to Go A-Sparkin' Oh, if you went to go a - s p a r k i n ' , I ' l l t e l l you where to go, Down on the creek, down here below, The l i t t l e kids a-crying with t h e i r heads not combed. Oh, they asked me t o dinner and I thought I ' d eat, They put i t on me t o carve up the meat, Give me an old knife without airy fork, Sawed half an hour and I couldn't make a mark. I sawed and I sawed and I got i t out of the plate, One of the g i r l s said, you'd better wait, I sawed and I sawed and I got i t on the floor, I gave i t a kick and I sent i t through the door. One of the girls said, You'd better run, Yonder comes dad with his double barreled gun, I jumped to the door j u s t as brave as a bear, And I tangled up my fingers in the old j a d e ' s hair. Oh, one of them g i r l s said, You'd b e t t e r run, I jumped t o the door just as brave as a bear, And I tangled up my f i n g e r s in the old man's h a i r. F i r s t thing they give me was an old grey horse, Already saddled f o r to throw my l eg across, I jumped in the saddle and I spurred him with my heel, And the crooked legged devil throwed me half across the f i e l d.Funding for digitization provided by the Arkansas Humanities Council and the Happy Hollow Foundation
        University of Arkansas: Digital Collections

        The use of volunteer leaders to support older adults in physically active leisure

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        A number of government reports have advocated the importance of healthy ageing and the need to develop multiple strategies to increase the physical activity levels of older Australians. One approach recommended is to use social support strategies to increase exercise adherence as well as improving health related outcomes. This study recruited a number of volunteer leaders (who were known by the acronym 'PAM' that stood for 'Physical Activity Motivator'). These volunteer leaders assisted and supported participants aged 65 years and older to participate in a community-based physical leisure activity. This activity was chosen by the older participant from an inventory of existing physical activity programs in the community. This paper reports on the effectiveness of strategies used to recruit volunteer leaders to help provide social support for older participants. In addition, it explores the volunteer leaders’ perceptions of the training program and the contribution volunteer leaders made in helping to achieve long term exercise adherence for older participants
        UQ eSpace (University of Queensland)

        Tests of Lepton Universality Using B-0 -> K(S)(0)l(+) l(-) and B+ -> K*(+)l(+)l(-) Decays

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        Tests of lepton universality in B-0 -> K(S)(0)l(+)l(-) and B+ -> K*(+)l(+)l(-) decays where l is either an electron or a muon are presented. The differential branching fractions of B-0 -> K(S)(0)e(+)e(-) and B+ -> K*(+)e(+)e(-) decays are measured in intervals of the dilepton invariant mass squared. The measurements are performed using proton-proton collision data recorded by the LHCb experiment, corresponding to an integrated luminosity of 9 fb(-1). The results are consistent with the standard model and previous tests of lepton universality in related decay modes. The first observation of B-0 -> K(S)(0)e(+)e(-) and B+ -> K*(+)e(+)e(-) decays is reported
        Archivio della Ricerca - Università di Pisa
        Archivio istituzionale della ricerca - Università di Bari
        ePubs: the open archive for STFC research publications
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        The Opinion – Volume 33, No. 1, August 1990

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        Table of Contents Nien Cheng to Kick Off Distinguished Speakers Series / Edie Michalski; Donn McLennen Love in the Law / Wiese/Olson Separate but Better Off? or is One Person, One Vote Still Valid? / Lowell J. Satre Jr. An Era of Strict Construction / Michael J. Varani A Proposal for More Effective Teaching at William Mitchell / Neil W. Hamilton Clinic Curriculum A Gold Mine of Opportunity / Resa Gilats One L; Who is This Cardozo Guy? / Mike Broback An Exclusive Interview with Chief Justice Warren E. Burger Editorial Board Richard J. Olsen (Editor in Chief); Karl Green; M. O\u27Sullivan Kane; Eric Douglas Larson; Tony Schertler; Tamara Tegeler; Robert Christensen; Tom Weiss; Richard K. Ellison; Mike Brobackhttps://open.mitchellhamline.edu/the-opinion/1113/thumbnail.jp
        Sussex Research Online

        Study of the Decays Ds+→KS0K+D_{s}^{+} \rightarrow K_{S}^{0}K^{+} and KL0K+K_{L}^{0}K^{+}

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        Using an e+e−e^+e^− annihilation data sample corresponding to an integrated luminosity of 3.19 fb−1^{−1} and collected at a center-of-mass energy s\sqrt{s} = 4.178 GeV with the BESIII detector, we measure the absolute branching fractions B(Ds+→KS0K+)=(1.425±0.038stat.±0.031syst.)%\mathcal{B}(D_{s}^{+} \rightarrow K_{S}^{0}K^{+}) = (1.425\pm0.038_{\rm stat.}\pm0.031_{\rm syst.})\% and B(Ds+→KL0K+)=(1.485±0.039stat.±0.046syst.)%\mathcal{B}(D_{s}^{+} \rightarrow K_{L}^{0}K^{+}) =(1.485\pm0.039_{\rm stat.}\pm0.046_{\rm syst.})\%. The branching fraction of Ds+→KS0K+D_{s}^{+} \rightarrow K_{S}^{0}K^{+} is compatible with the world average and that of Ds+→KL0K+D_{s}^{+} \rightarrow K_{L}^{0}K^{+} is measured for the first time. We present the first measurement of the KS0−KL0K_{S}^{0}-K_{L}^{0} asymmetry in the decays Ds+→KS,L0K+D_{s}^{+} \rightarrow K_{S,L}^{0}K^{+}, and R(Ds+→KS,L0K+)=B(Ds+→KS0K+)−B(Ds+→KL0K+)B(Ds+→KS0K+)+B(Ds+→KL0K+)=(−2.1±1.9stat.±1.6syst.)%R(D_{s}^{+} \rightarrow K_{S,L}^{0}K^{+})=\frac{\mathcal{B}(D_{s}^{+} \rightarrow K_{S}^{0}K^{+}) -\mathcal{B}(D_{s}^{+} \rightarrow K_{L}^{0}K^{+})}{\mathcal{B}(D_{s}^{+} \rightarrow K_{S}^{0}K^{+}) +\mathcal{B}(D_{s}^{+} \rightarrow K_{L}^{0}K^{+})}= (-2.1\pm1.9_{\rm stat.}\pm1.6_{\rm syst.})\%. In addition, we measure the direct CPCP asymmetries ACP(Ds±→KS0K±)=(0.6±2.8stat.±0.6syst.)%A_{\rm CP}(D_{s}^{\pm} \rightarrow K_{S}^{0}K^{\pm}) = (0.6\pm2.8_{\rm stat.}\pm0.6_{\rm syst.})\% and ACP(Ds±→KL0K±)=(−1.1±2.6stat.±0.6syst.)%A_{\rm CP}(D_{s}^{\pm} \rightarrow K_{L}^{0}K^{\pm}) = (-1.1\pm2.6_{\rm stat.}\pm0.6_{\rm syst.})\%
        IUScholarWorks Open

        Study of the Decays Ds+→KS0K+D_{s}^{+} \rightarrow K_{S}^{0}K^{+} and KL0K+K_{L}^{0}K^{+}

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        Using an e+e−e^+e^− annihilation data sample corresponding to an integrated luminosity of 3.19 fb−1^{−1} and collected at a center-of-mass energy s\sqrt{s} = 4.178 GeV with the BESIII detector, we measure the absolute branching fractions B(Ds+→KS0K+)=(1.425±0.038stat.±0.031syst.)%\mathcal{B}(D_{s}^{+} \rightarrow K_{S}^{0}K^{+}) = (1.425\pm0.038_{\rm stat.}\pm0.031_{\rm syst.})\% and B(Ds+→KL0K+)=(1.485±0.039stat.±0.046syst.)%\mathcal{B}(D_{s}^{+} \rightarrow K_{L}^{0}K^{+}) =(1.485\pm0.039_{\rm stat.}\pm0.046_{\rm syst.})\%. The branching fraction of Ds+→KS0K+D_{s}^{+} \rightarrow K_{S}^{0}K^{+} is compatible with the world average and that of Ds+→KL0K+D_{s}^{+} \rightarrow K_{L}^{0}K^{+} is measured for the first time. We present the first measurement of the KS0−KL0K_{S}^{0}-K_{L}^{0} asymmetry in the decays Ds+→KS,L0K+D_{s}^{+} \rightarrow K_{S,L}^{0}K^{+}, and R(Ds+→KS,L0K+)=B(Ds+→KS0K+)−B(Ds+→KL0K+)B(Ds+→KS0K+)+B(Ds+→KL0K+)=(−2.1±1.9stat.±1.6syst.)%R(D_{s}^{+} \rightarrow K_{S,L}^{0}K^{+})=\frac{\mathcal{B}(D_{s}^{+} \rightarrow K_{S}^{0}K^{+}) -\mathcal{B}(D_{s}^{+} \rightarrow K_{L}^{0}K^{+})}{\mathcal{B}(D_{s}^{+} \rightarrow K_{S}^{0}K^{+}) +\mathcal{B}(D_{s}^{+} \rightarrow K_{L}^{0}K^{+})}= (-2.1\pm1.9_{\rm stat.}\pm1.6_{\rm syst.})\%. In addition, we measure the direct CPCP asymmetries ACP(Ds±→KS0K±)=(0.6±2.8stat.±0.6syst.)%A_{\rm CP}(D_{s}^{\pm} \rightarrow K_{S}^{0}K^{\pm}) = (0.6\pm2.8_{\rm stat.}\pm0.6_{\rm syst.})\% and ACP(Ds±→KL0K±)=(−1.1±2.6stat.±0.6syst.)%A_{\rm CP}(D_{s}^{\pm} \rightarrow K_{L}^{0}K^{\pm}) = (-1.1\pm2.6_{\rm stat.}\pm0.6_{\rm syst.})\%
        IUScholarWorks (Indiana University)
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