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Deliverables and Services - IHP Microelectronics

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In Abb. 32 sind die wesentlichen Ergebnisse der elektrischen<br />

Messungen zusammengestellt. Die dielektrischen<br />

Konstanten der untersuchten Dielektrika werden in<br />

Abb. 32(a) mitein<strong>and</strong>er verglichen. Der k-Wert von monoklinem<br />

HfO 2 ist ungefähr 19 und somit in guter Übereinstimmung<br />

mit veröffentlichten Daten. Durch Hinzumischen<br />

von Ba kommt es zu einer leichten Erhöhung<br />

der Dielektrizitätskonstante, so dass ein Wert von ~ 23<br />

für amorphes BaHfO 3 erhalten wird. Die Kristallisation<br />

in die c-BaHfO 3 -Phase, nachgewiesen durch XRD, wird<br />

durch einen abrupten Anstieg der Dielektrizitätskonstante<br />

auf 38 begleitet.<br />

In Abb. 32(b) ist der Einfluss der RTA-Beh<strong>and</strong>lung auf<br />

die Leckströme in BaHfO 3 -Proben dargestellt. Amorphe<br />

BaHfO 3 -Schichten erfüllen die DRAM-Leckstromerfordernisse<br />

(J < 10 -8 A / cm 2 @ 1 V) für CET-Werte herunter<br />

bis zu ~ 2 nm. Die RTA-induzierte Kristallisation<br />

dieser Schichten ergibt eine signifikante Verringerung<br />

von CET infolge einer verbesserten Dielektrizitätskonstante<br />

und einer Verdichtung der dielektrischen Schicht.<br />

Abb. 32: Vergleich zwischen m-HfO 2 , a-BaHfO 3 und c-BaHfO 3 .<br />

Fig. 32: Comparison between m-Hfo 2 , a-BaHfo 3 , <strong>and</strong> c-BaHfo 3 .<br />

A U S G E w ä H L T E P R O J E K T E – S E L E C T E d P R O J E C T S<br />

In Fig. 32, the main results of the electrical measurements<br />

are summarized. the dielectric constants of<br />

the investigated dielectrics are compared in Fig.<br />

32(a). the k-value of the monoclinic Hfo 2 is approx.<br />

19, which is in good agreement with published data.<br />

Admixture of Ba results in a slight increase of the<br />

permittivity yielding a value of approx. 23 for amorphous<br />

BaHfo 3 . Crystallization in the c-BaHfo 3 phase<br />

detected by XRD is accompanied by an abrupt increase<br />

of the dielectric constant to 38.<br />

In Fig. 32(b), the influence of the RtA treatment on<br />

leakage currents in BaHfo 3 samples is shown. Amorphous<br />

BaHfo 3 layers meet the DRAM leakage current<br />

requirement (J < 10 -8 A / cm 2 @ 1 V) for Cet values<br />

down to approx. 2 nm. RtA induced crystallization of<br />

these films results in a significant reduction of the<br />

Cet due to improved dielectric constant <strong>and</strong> densification<br />

of the dielectric film. At the same time, however,<br />

a substantial increase in the leakage current density<br />

is observed. leakage current characteristics of<br />

thin c-BaHfo 3 layers were further investigated using<br />

temperature dependent measurements summarized<br />

in Fig. 33 showing leakage JV curves measured for<br />

an about 8 nm thick film at different temperatures<br />

under tin substrate injection. the currents detected<br />

at lower voltages are noisy <strong>and</strong> show only weak temperature<br />

dependence. Given the voltage dependence<br />

<strong>and</strong> the magnitude of these currents, we suppose that<br />

they are associated with macroscopic defects (“hot<br />

spots”), but any specific characterization of these defects<br />

is difficult at this stage of research. on the other<br />

h<strong>and</strong>, it seems to be clear that leakage currents in the<br />

higher voltage range are dominated by point defects<br />

presumably also associated with some hot spot areas.<br />

In this strongly temperature dependent leakage regime,<br />

the concentration of carriers is determined by<br />

carrier trapping <strong>and</strong> detrapping, with voltage dependence<br />

resembling a poole-Frenkel process.<br />

A n n u A l R e p o R t 2 0 0 7<br />

6

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