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PHYS07200604007 Manas Kumar Dala - Homi Bhabha National ...

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Electronic Structure of Ca 0.86 Pr 0.14 MnO 3 100<br />

Intensity (arb. units)<br />

A<br />

30 K<br />

70 K<br />

110 K<br />

220 K<br />

300 K<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

-0.2<br />

Binding Energy (eV)<br />

Figure 5.2: The high resolution spectra of the near E F region of the valence band of<br />

Ca 0.86 Pr 0.14 MnO 3 for 30 K, 70 K, 110 K, 220 K and 300 K. This feature refers to the<br />

e g band.<br />

states due to the Mn 3d - O 2p hybridization. The broad feature appearing at ∼ 6 eV<br />

(marked D) is due to the bonding states of this hybridization while its non-bonding<br />

states appear as a shoulder at ∼ 3.2 eV (marked C). The peak at ∼ 2 eV (marked B)<br />

is due to the Mn 3d t 2g states of the MnO 6 octahedra [17]. The Mn 3d e g↑ states of<br />

the octahedra appear around ∼ 0.3 eV (marked A) in the spectra. It should be noted<br />

that the intensity of the peak B decreases with decrease of temperature while that of<br />

the feature A increases. These spectral weight shifts are characteristic of many CMR<br />

systems. The e g states lying close to the E F are important for the conductivity of this<br />

material. A high resolution spectra of the near E F region is presented in figure 5.2.<br />

As the temperature is lowered from 293 K the feature A starts appearing. Further,<br />

below the transition temperature T c (110 K), the intensity of A steeply increases and<br />

goes through a maximum. The 30 K spectrum again shows a smaller intensity for<br />

this feature compared to the one at 70 k. Interestingly, below the T c , the leading<br />

edges of the different spectra move towards the E F as we go down in temperature.

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