Name Extraction and Translation for Distillation

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Description

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Name Extraction and Translation for Distillation Heng Ji and Ralph Grishman New York University Dayne Freitag, Matthias Blume and Zhiqiang (John) Wang Fair Isaac Corp. Shahram Khadivi, Richard Zens and Hermann Ney RWTH Abstract Name translation is important well beyond the relative frequency of names in a text: a cor- rectly translated passage, but with the wrong name, may lose most of its value. The Night- ingale team has built a name translation com- ponent which operates in tandem with a con- ventional phrase-based statistical MT system, identifying names in the source text and pro- posing translations to the MT system.

• asian person names by pinyin
• person names from the reference translations of refer- ence transcripts
• men- tion translations
• person names
• corpus
• phrase
• translation
• word
• names
• name

Sujets

• Bender
• Farber
• Kalmar
• Word sense disambiguation
• Gonzalo
• Linguistic Data Consortium
• Paulson

Informations

• Publié par: usse0
• Nombre de lectures: 27
• Langue: English

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“and the incline is frictionless”

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Errata for: Tipler,Physics for Scientists and Engineers, 5/e Volume One Paperback Version This version has been replaced by a corrected Vol. 1 (Hardback) and Vol. 1A and 1B (Paperbacks) .

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Chapter One

Chapter Two

nd Pg. 15; Problem 42; 2 line.

Chapter Four

Page 1

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Wiley Coyote Wile E. Coyote

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Chapter Three

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Chapter Five

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Chapter Six

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Chapter Seven

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weight. weight, which is about 650 N.

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Chapter Eight

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Chapter Nine

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st nd th The errors in the original figure were in the 1 , 2 and 4 places of the top row.

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G L t f L tz G L t f L k  t z

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complete

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Chapter Fourteen

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Chapter Eighteen

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Appendix A

Appendix D

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Physical Constants; Bohr Magneton.

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400 m/s If we let the lengthLof the tube be 1.2 m and assume thatu air = 344 m/s (the speed of sound in air at 20ºC), th then the 10 harmonic corresponds toD= 25.3 cm and a driving frequency of 680 Hz.

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Chapter Twenty

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IfL= 1.2 m, then (neglecting end effects) a resonance will be observed forλ= 10 cm, corresponding to the third harmonic of the resonance frequency. Ifu= 400 m/s, the frequency should be 4000 Hz. For the fundamental mode, the only displacement antinode appears to be at the open end of the tube and end effects need to be considered. (See Example 16-9.) Iff= 2 kHz andu He = 1008 m/s (the speed of sound th in helium at 20û), theDfor the 10 harmonic in helium would be 8.60 cm. Hence, neglecting end effects at the driven end, a tube whose length is the least common multiple of 8.60 cm and 25.3 cm (218 cm) would work well for the measurement of the speed of sound in either air or helium.

Chapter Eighteen

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