Fission of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Es</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>2</mml:mn><mml:mn>5</mml:mn><mml:mn>5</mml:mn><mml:mo>,</mml:mo><mml:mn>2</mml:mn><mml:mn>5</mml:mn><mml:mn>6</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>,<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Fm</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>2</mml:mn><mml:mn>5</mml:mn><mml:mn>5</mml:mn><mml:mo>−</mml:mo><mml:mn>2</mml:mn><mml:mn>5</mml:mn><mml:mn>7</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>, and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Md</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>258</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>at moderate excitation energies

The fission of $^{255,256}\mathrm{Es}$, $^{255\ensuremath{-}257}\mathrm{Fm}$, and $^{258}\mathrm{Md}$ has been studied in the excitation energy range from threshold to 25 MeV. A target of $^{254}\mathrm{Es}$ was used in the direct reaction studies; (d,$\mathrm{p}f$), (t,$\mathrm{p}f$), ($^{3}\mathrm{He}$,$\mathrm{d}f$), ($^{3}\mathrm{He}$,$\mathrm{p}f$), and in the compound induced fission reactions formed with p, d, t, and $\ensuremath{\alpha}$ particle projectiles. Coincident fission fragment energies were recorded along with (in the direct reaction studies) the outgoing light charged particle. The mass and kinetic energy distributions were studied as a function of nuclear excitation energy. The observed bulk properties were consistent with established systematics in that they exhibited an asymmetric mass distribution and a phenomenologically consistent total kinetic energy. However, the systems demonstrated a fission decay mode which we ascribe to high energy symmetric fission decay. This component, though somewhat arbitrary in its definition, showed a general decrease in yield as a function of increasing nuclear excitation energy. This observed rapid change in fission properties between "normal" and high energy symmetric fission probably points to the important observable consequences that can occur from small variations in the potential energy surface.

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