Statistical properties of the well deformed <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi>Sm</mml:mi><mml:mprescripts /><mml:none /><mml:mrow><mml:mn>153</mml:mn><mml:mo>,</mml:mo><mml:mn>155</mml:mn></mml:mrow></mml:mmultiscripts></mml:math> nuclei and the scissors resonance

The nuclear level densities (NLDs) and the $\ensuremath{\gamma}$-ray strength functions ($\ensuremath{\gamma}\mathrm{SFs}$) of $^{153,155}\mathrm{Sm}$ have been extracted from ($d,p\ensuremath{\gamma}$) coincidences using Oslo method. experimental NLD $^{153}\mathrm{Sm}$ is higher than $^{155}\mathrm{Sm}$, in accordance with microscopic calculations. $\ensuremath{\gamma}\mathrm{SFs}$ are fair agreement QRPA calculations based on D1M Gogny interaction. An enhancement observed $\ensuremath{\gamma}\mathrm{SF}$ for both nuclei around 3 MeV excitation energy attributed to $M1$ scissors resonance (SR). Their integrated strengths were found be range 1.3--2.1 4.4--6.4 ${\ensuremath{\mu}}_{N}^{2}$ respectively. SR $^{155}\mathrm{Sm}$ comparable those deformed even-even Sm isotopes fluorescence measurements, while that lower expected.