Fred Hoyle - Source Counts - Steady State Cosmology Historical Radio Astronomy 27 Aug 2012 IAU GA Beijing Ron Ekers CSIRO, Australia 1.

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Presentation transcript:

Fred Hoyle - Source Counts - Steady State Cosmology Historical Radio Astronomy 27 Aug 2012 IAU GA Beijing Ron Ekers CSIRO, Australia 1

Summary n My involvement with Hoyle & Ryle in 1969 n The controversy n History of source counting n The radio luminosity function and how it can mess everything up n Evolution of radio surveys over time –Livingston curves 2

Early views on cosmology and radio sources n Steady State was the favored cosmology –Testable theory –Charismatic advocates (Gold, Hoyle …… n Big Bang –a popular term coined by Fred Hoyle n Hoyle and Burbidge were early supporters of the extra galactic radio source models n Super massive stars (not blackholes) in centres of galaxies n Opposed the radio star interpretation and already in conflict with Ryle 3

History of source counting n Ryle measures a cumulative source count slope steeper than S -1.5 –Concludes that the universe is evolving –Initially S -2.5 and later revised to S -1.8 –Peter Scheuer understood the confusion issue n Mills obtains a slope less than S -1.5 –Measured S -1.8 and corrected it to S -1.5 (resolution bias) –Concludes that the universe is consistent with static Euclidean or steady state. –May have been misled by the number of bright extended SH sources n Hoyle argues that Ryle is wrong and that counting sources can’t say anything about cosmology –I worked with Hoyle between 1969 and 1970 n All were wrong in different ways! –Source counting gets a bad reputation 4

Radio Source Counts 5

Role of the Radio Luminosity Function n What is the relationship between flux density and distance? –Naively you expect weaker sources to be further away but … n The critical luminosity function –  (P)  P -3/2 (Static Euclidean) –Applies for a large range in radio luminosity –Eg van Hoerner ApJ 186, 741 (1973) n Hubble relation, an inverse Hubble relation or no relation between flux density and distance 6

Radio Luminosity Function 7 Volume n Local Bivariate RLF –B2 radio survey n Auriemma et al A&A 57, (1977)

Role of the Radio Luminosity Function (2) n What is the relationship between flux density and distance? –Naively you expect weaker sources to be further away but … n The critical luminosity function –  (P)  P -3/2 (Static Euclidean) –Applies for a large range in radio luminosity –Eg van Hoerner ApJ 186, 741 (1973) n Hubble relation, an inverse Hubble relation or no relation between flux density and distance 8

The radio luminosity function n For a flux limit S min –we see out to R=(P/S min ) 0.5 –ie in a Volume V  ((P/S min ) 1.5 n If the RLF  (P)  P  –Then the number of sources  P . (P/S min ) 1.5 n Hence 3 possibilities: –   -1.5 as P increases N increases »More sources at greater distance –  = -1.5 any P is equally probable »Flux density is independent of distance –   -1.5 as P increases N decreases »More sources at smaller distance 9

Hoyle 1970 n Hoyle & Burbidge, Nature 227, (1970) –the data supports a differential luminosity function of the form dL/L 5/2 n They then go on to show that there is no relation between flux density and redshift n Van Hoerner, ApJ 186, (1973) –Introduces concept of a critical luminosity function –Discusses the evolution of the rlf –eg density v luminosity evolution 10

Fred’s Institute (IoTA) in 1969 n Across Madingly Road from the Cavendish Laboratory n A few of us crossed the road –Foreigners –Peter Scheuer –Martin Rees n Atmosphere was very different n Fred’s circus – many visitors n Open v Closed n Fred supported my experiment at Algonquin Park to search for CMB fluctuations (1969) 11

Evolution of radio surveys 12 n Increase by 10 5 in 60 yr n 3 year doubling time for survey size n Exponential? n What happened from 1970 to 1990? –WSRT and VLA focus on individual objects n Tracks telescope sensitivity evolution

11 Aug 2009IAU GA XXVII SpS5 Radio Telescope Sensitivity n Exponential increase in sensitivity x 10 5 since 1940 ! –3 year doubling time for sensitivity n Follows the well known law of exponential growth in Science

14 Exponential Growth n Livingstone Curve –Blewett, Brookhaven 1950 –Fermi 1954 –Livingstone 1962 n De Solla Price 1963 –exponential growth –Little science, big Science