Hello everybody. I speak about number of states. Operation number of state per letter. Equal number of level per MEV is level density. Because the state density number of state per MEV. There are two ways to obtain for a training that you will get experimental or theoretical approach. The theoretical method is that's the common method. There are various experimental approaches such as counting of neutron resonance, trivial counting, vibration spectra-hostle, or metal. But we compare our results by experimental data by the hostle. The statistical method is based on the theoretical method. The partial function is based on the statistical method. One is the system of eigenvalue E1, E2. The partial function is the equivalent formula. We have a state density and we have a lot of transform of the partial function for state density. We apply the standard point method and we have the state density. If the state only asking by the energy and angular momentum or some quantum number, we have grand partial function and the same way we apply the set of point condition and we have state density. The state density for single type of fermion is a well exponential entropy. The determinant of the second derivation of the partial function taken at the standard point. And we have a state density per-operation number of state-care level. And we have a level density. That sigma square is the speed cut of parameter. We have microscopic formula and the tau-1 described this microscopic model because the entropy doesn't increase as smoothly as was explained with microscopic theory or it's independent. We speak about the BCS or microscopic method. The Fermi-gas method model which is used in the data analysis has very little fiscal significance. This model ignored the pairing traction between natural and also an awesome natural energy level to be the quality. But we have extracted the natural wave density with inclusion of using a superconductive tool with inclusion and natural pairing interaction. This model is more physical in that in addition to taking into a compound interaction it's awesome or realistic single-part energy level by the paper in this value of the partial vectorial surface. The grand partial function method is used for this approach due to the algorithm of this function is G-sparing function. The initial quantity is needed to solve before equation the ground state gap carbon dioxide is needed to solve before equation the ground state gap carbon dioxide is used in the pairing of strange from equation 11 or we use the atomic mass evaluation. In the performance of the state and the energy of the single particle level first obtained from the Nielsen potential. The calculation has been based on the modified formula or according to Nielsen potential for the form NTI. In this field the single particle, proton single particle level and Nielsen single particle level show you for D-Y-Y-6-O. Now we have a calculation have been known in the following way the ground state energy of the first calculate by the T-equation 0 and so we solve the equation 2 and 6 for lambda and G for given if your number N pairing energy the obtained from equation 11 or atomic mass evaluation. The gap parameter for Nielsen system and proton system show and the critical temperature for FE is 0.69MV. And experimental data by the Oslo group and always this calculation is 0 and the oral argument is satisfactory. The expectation energy as a function of temperature and on the on-thrope as a function of temperature is present. And we see the pair breaking in critical temperature and in the entropy figure. Or in after-faker in PRC we calculate the Nielsen density entropy and we introduce the ratio of neutron proton entropy excess in SN121 compared to SN122 in this paper. And for example we have experiment between experimental and theoretical data. The experimental data from the Oslo group, Oslo method. And the ratio of neutron and proton entropy excess is discussed. The role of neutron and proton in this figure show is shown and the proton system of proton pressure play a minor role as expected. Or in recent paper we roll out the neutron and proton entropy excess in cut-off and momentum in a show are discussed. In this paper the experimental and theoretical calculation for the density is present. And finally we show the result for dy160. In this figure the excitation has the function of nuclear temperature. And critical temperature is about 0.546MAD. And finally we have nuclear density as a function of excitation energy. The experimental data is from by the Oslo group and got Hermes and Kiske-Ribius C. And the field star in the field is the calculation. Or the system is the calculation. Some are in conclusion. And important going in nuclear physics to trace them. You know, quantity has the function of excitation energy. The level density has a function of excitation energy is the starting point to extract 10 million-cap quantities such as entropy temperature and etc. Do not get the level density and entropy having calculated for the Y and the previous one the DCS-Hammitronian with the inclusion of the Tracking Permune, with the Nielsen-Welz gene. The results show that the experimental redundancy are Wheeler-Precius. But we found quenching of air in Gafnir the critical temperature. The thermal breaking of Cooper-Precius to increasing entropy on the valedence tip. The single-volans, single particle entropy are determined from the mass entropy compared to even neighbor nucleus. And the ratio of neutron and proton entropy excess are de-Germany. Thank you for your