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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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In the right panel is given the results at finitetemperature (T = 20MeV). We find that the EOS of ANM fulfills satisfactorily a quadratic dependence on ...

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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Left panel: the energy per nucleon of SNM vs. density. ... 2 the isovector part of the EOS as a function of β2, where β is the isospin asymmetry of ANM.

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