- Albayrak, I;
- Mamyan, V;
- Christy, ME;
- Ahmidouch, A;
- Arrington, J;
- Asaturyan, A;
- Bodek, A;
- Bosted, P;
- Bradford, R;
- Brash, E;
- Bruell, A;
- Butuceanu, C;
- Coleman, SJ;
- Commisso, M;
- Connell, SH;
- Dalton, MM;
- Danagoulian, S;
- Daniel, A;
- Day, DB;
- Dhamija, S;
- Dunne, J;
- Dutta, D;
- Ent, R;
- Gaskell, D;
- Gasparian, A;
- Gran, R;
- Horn, T;
- Huang, Liting;
- Huber, GM;
- Jayalath, C;
- Johnson, M;
- Jones, MK;
- Kalantarians, N;
- Liyanage, A;
- Keppel, CE;
- Kinney, E;
- Li, Y;
- Malace, S;
- Manly, S;
- Markowitz, P;
- Maxwell, J;
- Mbianda, NN;
- McFarland, KS;
- Meziane, M;
- Meziani, ZE;
- Mills, GB;
- Mkrtchyan, H;
- Mkrtchyan, A;
- Mulholland, J;
- Nelson, J;
- Niculescu, G;
- Niculescu, I;
- Pentchev, L;
- Puckett, A;
- Punjabi, V;
- Qattan, IA;
- Reimer, PE;
- Reinhold, J;
- Rodriguez, VM;
- Rondon-Aramayo, O;
- Sakuda, M;
- Sakumoto, WK;
- Segbefia, E;
- Seva, T;
- Sick, I;
- Slifer, K;
- Smith, GR;
- Steinman, J;
- Solvignon, P;
- Tadevosyan, V;
- Tajima, S;
- Tvaskis, V;
- Vulcan, WF;
- Walton, T;
- Wesselmann, FR;
- Wood, SA;
- Ye, Zhihong
We present extractions of the nucleon nonsinglet moments utilizing new precision data on the deuteron F_{2} structure function at large Bjorken-x determined via the Rosenbluth separation technique at Jefferson Lab Experimental Hall C. These new data are combined with a complementary set of data on the proton previously measured in Hall C at similar kinematics and world datasets on the proton and deuteron at lower x measured at SLAC and CERN. The new Jefferson Lab data provide coverage of the upper third of the x range, crucial for precision determination of the higher moments. In contrast to previous extractions, these moments have been corrected for nuclear effects in the deuteron using a new global fit to the deuteron and proton data. The obtained experimental moments represent an order of magnitude improvement in precision over previous extractions using high x data. Moreover, recent exciting developments in lattice QCD calculations provide a first ever comparison of these new experimental results with calculations of moments carried out at the physical pion mass, as well as a new approach that first calculates the quark distributions directly before determining moments.