1. Convolution regularization and gauge invariance, C. Lopez and E. Mendel, Lett. Nuovo Cimento 19, 201 (1977).

2. Functional equations for path dependent phase factors in Yang-Mills theories, L. Durand and E. Mendel, Phys. Lett. 85 B, 241 (1979).

3. Gauge theories and phase factors in the coordinate gauge, L. Durand and E. Mendel, Proc. of the II Chilean Symposium on theoretical Physics, Santiago 1980.

4. Field strength formulation of gauge theories: Transformation of the functional integral, L. Durand and E. Mendel, Phys. Rev. D 26, 1368 (1982).

5. Field strength formulation of gauge theories: The Hamiltonian approach in the Abelian theory, E. Mendel and L. Durand, Phys. Rev. D 30, 1754 (1984).

6. Semiclassical calculation of the photoproduction of breather modes in the Sine-Gordon theory, N. Weiss, E. Mendel and A.J. Berlinsky, Can. J. Phys. 62, 616 (1984).

-. Monte Carlo simulation of the excitation of breather modes in the Sine-Gordon theory, E. Mendel and N. Weiss,in preparation.

7. Hadronic structure using lattice QCD with Chemical Potential, E. Mendel. Technion Preprint, TECHNION-PH-86-16, March 1986.

8. Hadronic structure by introducing Chemical Potential, E. Mendel, Nuclear Physics B4 (Proc. Suppl.), 308, (1988).

9. QCD at finite Chemical Potential, E. Mendel, Nucl. Phys. B9 (Proc. Suppl.), 347, (1989).

10. Nucleon degeneracy on the lattice explains early baryon density onset, E. Mendel, Nucl. Phys. B20 (Proc. Suppl.), 343, (1991).

11. Finite Baryon Density in lattice simulations and nuclear matter, E. Mendel, Nucl. Phys. B387, 485, (1992).

12. Path integral formalism for a simple interacting nucleon model, E. Mendel, Nucl. Phys. B30 (Proc. Suppl.), 944, (1993).

13. Extrapolation to nature of finite baryon density lattice results using quantum Monte Carlo, E. Mendel, Nucl. Phys. B34 (Proc. Suppl.), 304, (1994).

14. Negative-energy spinors and the Fock space of lattice fermions at finite chemical potential, E. Mendel and L. Polley, Z. Phys. C 65, 127 (1995).

15. QCD at finite baryon density with t-asymmetric fermions, E. Mendel and L. Polley, Nucl. Phys. B42 (Proc. Suppl), 535, (1995). ( hep-lat@ftp.scri.fsu.edu : 9501012).

16. Finite density results for Wilson fermions using the volume method, W. Wilcox, S. Trendafilov and E. Mendel, Nucl. Phys. B42 (Proc. Suppl), 557 (1995). (hep-lat: 9501011)

17. Simple quantum mechanical phenomena and the Feynman real time path integral, A. Dullweber, E. Hilf and E. Mendel, Oldenburg prep. UO-Phys-Theo, 28 Nov. 1995. ( quant-ph@xxx.lanl.gov : 9511042). Submitted to Phys. Lett. A.

18. Observing instantons directly on the lattice without cooling, E. Mendel and G. Nolte, Oldenburg prep. UO-Phys-Theo, 29 Nov. 1995, ( hep-lat: 9511030). Submitted to Phys. Rev. D .

19. Extended instantons generated on the lattice, E. Mendel and G. Nolte, Nucl. Phys B53.(Proc. Suppl.) (1997) 567 , ( hep-lat: 9608060).

-. Generating smooth instantons for SU(2), E. Mendel, in preparation.

20. Nonperturbative real time propagation at finite temperature, E. Mendel and M. Nest, Nucl. Phys B63. (Proc. Suppl) (1998) 445. (hep-lat/9709144).

21. Can a flavour conserving treatment improve things? E. Mendel, Nucl. Phys. A642 (1998) 282. (hep-lat/9807004)

22. Time evolution for quantum systems at finite temperature, E. Mendel and M. Nest, Nucl. Phys. B562 (1999) 567, (hep-th/9807030).

23. Real time correlations at finite temperature for the Ising model, E. Mendel, Nucl. Phys. B73 (Proc. Suppl.)(1999) 778, (hep-th/9810160)