Curvature of the Universe from Cosmic Microwave Background Fluctuations

Similar documents
Formation of the Universe. What evidence supports current scientific theory?

Modern Cosmology April 4, Lecture 3 1

Lecture 37 Cosmology [not on exam] January 16b, 2014

The Cosmic Microwave Background

Assignments. Read all (secs ) of DocOnotes-cosmology. HW7 due today; accepted till Thurs. w/ 5% penalty

Lecture #24: Plan. Cosmology. Expansion of the Universe Olber s Paradox Birth of our Universe

Cosmology. Thornton and Rex, Ch. 16

The SDSS-III Baryon Acoustic Oscillation Survey (BOSS)

The Big Bang The Beginning of Time

Cosmology. An Analogy 11/28/2010. Cosmology Study of the origin, evolution and future of the Universe

The Cosmic Microwave Background

Inflation; the Concordance Model

Inflationary Universe and. Quick survey about iclickers Review of Big Bang model of universe Review of Evidence for Big Bang Examining Inflation

Survey questions. Inflationary Universe and. Survey Questions. Survey questions. Survey questions

Chapter 22 Lecture. The Cosmic Perspective. Seventh Edition. The Birth of the Universe Pearson Education, Inc.

What is the evidence that Big Bang really occurred

The Expanding Universe

Chapter 21 Evidence of the Big Bang. Expansion of the Universe. Big Bang Theory. Age of the Universe. Hubble s Law. Hubble s Law

Astronomy 182: Origin and Evolution of the Universe

The Standard Big Bang What it is: Theory that the universe as we know it began billion years ago. (Latest estimate: 13:82 ± 0:05 billion years!)

Chapter 23 The Beginning of Time. Agenda. Presentation Tips. What were conditions like in the early universe? 23.1 The Big Bang.

Cosmology. Clusters of galaxies. Redshift. Late 1920 s: Hubble plots distances versus velocities of galaxies. λ λ. redshift =

Planetarium/Observing: the clock is ticking! Don t forget to fill out your Planetarium/ Observing impression online.

Lecture 03. The Cosmic Microwave Background

A5682: Introduction to Cosmology Course Notes. 11. CMB Anisotropy

Module 3: Astronomy The Universe Topic 1 Content: Cosmology Presentation Notes

Cosmic Microwave Background. Eiichiro Komatsu Guest Lecture, University of Copenhagen, May 19, 2010

THE UNIVERSE CHAPTER 20

The oldest science? One of the most rapidly evolving fields of modern research. Driven by observations and instruments

The Beginning of the Universe 8/11/09. Astronomy 101

v = H o d Hubble s Law: Distant galaxies move away fastest Velocity (v) is proportional to Distance (d):

Implications of the Hubble Law: - it is not static, unchanging - Universe had a beginning!! - could not have been expanding forever HUBBLE LAW:

Cosmology and the Evolution of the Universe. Implications of the Hubble Law: - Universe is changing (getting bigger!) - it is not static, unchanging

The expansion of the Universe, and the big bang

Taking the Measure of the Universe. Gary Hinshaw University of British Columbia TRIUMF Saturday Series 24 November 2012

Astronomy 162, Week 10 Cosmology Patrick S. Osmer Spring, 2006

9.2 The Universe. p. 368

Galaxy A has a redshift of 0.3. Galaxy B has a redshift of 0.6. From this information and the existence of the Hubble Law you can conclude that

3. It is expanding: the galaxies are moving apart, accelerating slightly The mystery of Dark Energy

The Formation of the Solar System

Cosmology. Big Bang and Inflation

The first 400,000 years

Astr 102: Introduction to Astronomy. Lecture 16: Cosmic Microwave Background and other evidence for the Big Bang

Modern Physics notes Spring 2005 Paul Fendley Lecture 38

Physics Nobel Prize 2006

Astr 2320 Thurs. May 7, 2015 Today s Topics Chapter 24: New Cosmology Problems with the Standard Model Cosmic Nucleosynthesis Particle Physics Cosmic

The Big Bang Theory was first proposed in the late 1920 s. This singularity was incredibly dense and hot.

Midterm. 16 Feb Feb 2012

Astronomy: The Big Picture. Outline. What does Hubble s Law mean?

The Early Universe: A Journey into the Past

Cosmology. Chapter 18. Cosmology. Observations of the Universe. Observations of the Universe. Motion of Galaxies. Cosmology

o Terms to know o Big Bang Theory o Doppler Effect o Redshift o Universe

Chapter 18. Cosmology in the 21 st Century

A100H Exploring the Universe: Big Bang Theory. Martin D. Weinberg UMass Astronomy

Lecture Outlines. Chapter 26. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc.

Lecture 12. Inflation. What causes inflation. Horizon problem Flatness problem Monopole problem. Physical Cosmology 2011/2012

The Early Universe: A Journey into the Past

Lab #10 Atomic Radius Rubric o Missing 1 out of 4 o Missing 2 out of 4 o Missing 3 out of 4

Chapter 18. Cosmology. Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

Prelab 9: The Hubble Redshift Distance Relation

Astronomy 102 Lab: Hubble Law

Cosmic Microwave Background

The Dawn of Time - II. A Cosmos is Born

Brief Introduction to Cosmology

AST207 F /1/2010

Final Exam. String theory. What are these strings? How big are they? Types of strings. String Interactions. Strings can vibrate in different ways

The Cosmic Microwave Background

Announcements. Homework. Set 8now open. due late at night Friday, Dec 10 (3AM Saturday Nov. 11) Set 7 answers on course web site.

CH 14 MODERN COSMOLOGY The Study of Nature, origin and evolution of the universe Does the Universe have a center and an edge? What is the evidence

3 Observational Cosmology Evolution from the Big Bang Lecture 2

Assignment #0 Using Stellarium

STUDY OF THE LARGE-SCALE STRUCTURE OF THE UNIVERSE USING GALAXY CLUSTERS

Chapter 22 Back to the Beginning of Time

COSMOLOGY The Universe what is its age and origin?

Galaxies 626. Lecture 3: From the CMBR to the first star

AST5220 lecture 2 An introduction to the CMB power spectrum. Hans Kristian Eriksen

Chapter 23 Lecture. The Cosmic Perspective Seventh Edition. Dark Matter, Dark Energy, and the Fate of the Universe Pearson Education, Inc.

1920s 1990s (from Friedmann to Freedman)

Expanding Universe. 1) Hubble s Law 2) Expanding Universe 3) Fate of the Universe. Final Exam will be held in Ruby Diamond Auditorium

Astroparticle physics

Island Universes. Up to 1920 s, many thought that Milky Way encompassed entire universe.

The Big Bang Theory. Rachel Fludd and Matthijs Hoekstra

Connecting Quarks to the Cosmos

BIG BANG SUMMARY NOTES

Chapter 27: The Early Universe

The best evidence so far in support of the Big Bang theory is:

History of the Universe Unit Tracking Sheet

OUSSEP Final Week. If we run out of time you can look at uploaded slides Pearson Education, Inc.

Lecture 09. The Cosmic Microwave Background. Part II Features of the Angular Power Spectrum

Lecture PowerPoints. Chapter 33 Physics: Principles with Applications, 7 th edition Giancoli

The cosmic background radiation II: The WMAP results. Alexander Schmah

Testing the Big Bang Idea

Origin of the Universe

Cosmic Background Radiation

A5682: Introduction to Cosmology Course Notes. 11. CMB Anisotropy

n=0 l (cos θ) (3) C l a lm 2 (4)

What forms AGN Jets? Magnetic fields are ferociously twisted in the disk.

Chapter 26 Cosmology II Future and Issues

VU lecture Introduction to Particle Physics. Thomas Gajdosik, FI & VU. Big Bang (model)

Lecture 34. General relativity

Transcription:

Curvature of the Universe from Cosmic Microwave Background Fluctuations Introduction Daniel M. Smith, Jr., South Carolina State University, dsmith@scsu.edu The Big Bang Theory that explains the creation, contents, and evolution of the universe is a scientific theory, a theory that can be proved wrong. The overwhelming evidence, however, is that the theory is a correct description of the universe. This lab explores one consequence of the existence of radiation from the extraordinarily hot beginning of the universe fluctuations in the radiation indicate that the universe was not perfectly smooth initially. In the very early universe there are no atoms; charged electrons and protons scatter light continuously as the universe expands and cools. Eventually, 380,000 years after the Big Bang, the universe cools enough for neutral atoms (H and He) to form and light no longer scatters. But light that scattered just as the neutral atoms were formed continues to travel, virtually unimpeded, and it can be observed today as microwaves of temperature 2.7 K ( 454.8 F) along with the temperature fluctuations due to the scattering. Studying the temperature fluctuations will allow you to draw conclusions about the shape and contents of the universe. Outline of Activities Temperature Fluctuations in the Cosmic Microwave Background (CMB) Goals: Plot theoretical maps of temperature fluctuations and power spectra for varying amounts of curvature in the universe, and compare the maps to the observed universe. Curvature of the Universe and Temperature Fluctuations in the CMB Cosmologists have observed and recorded the microwave fluctuations and converted them to a temperature map and a particular kind of graph called a power spectrum. You will discover the curvature of the universe its shape by comparing observations to the temperature map and power spectrum generated from Big Bang s theoretical predictions. To understand what is meant by curvature of the universe, examine the trajectory of the light (indicated by lines) from two stars in the zero (flat), positive (closed), and negative (open) curvature universes below. The black dots in the diagrams represent where the stars are observed. Zero curvature = flat universe, Positive curvature = closed universe, Negative curvature = open universe Question 1. For the open universe, when observations are made (at the black dots), will the two stars appear to be closer together or farther apart than their actual separation distance?

2 Question 2. For the closed universe, when observations are made (at the black dots) will the two stars appear to be closer together or farther apart than their actual separation distance? Directions 1. The temperature map generated by theory is in a FITS format favored by astronomers, so you need additional software to view your Big Bang predictions. Go to the website http://hea-www.harvard.edu/rd/ds9/site/home.html and click the download link to install the DS9 viewer (JS9 is available as an alternative). 2. Go to the website http://lambda.gsfc.nasa.gov/toolbox/tb_camb_form.cfm to generate the theoretical temperature maps and power spectra. Choose Sky Map Output: Temperature Only, Beam Size (arcmin) 13.5, and Synfast Random # Seed 2735. (The Seed insures that the random number generator starts at the same value every time, important for making comparisons, so another value can be set other than 2735 but whatever value is chosen must be used throughout the lab.) You will explore what happens as a result of changing Ω k, the curvature parameter. Set it to Ω k = 0 (flat universe), then press Go at the bottom of the page. 3. After a while, a page of Output from CAMB will be returned. From that page, record Om_K, Age of universe, Om_Lambda, and Om_m in the table below, for the flat universe. From the output page, also download a file that has a name similar to camb_98150569_mollweide_map_.fits, and the graph C l TT vs. l. Be sure to save the mollweide map with the a.fits suffix, and include the label K0 in the file names when they are saved. 4. Refresh the camb_form web page, then repeat steps 2 and 3, but with Ω k = +0.4 (open universe * ). Be sure to keep the seed value the same as before. Include the label K.4 in the two file names when they are saved. 5. Refresh the camb_form web page, then repeat steps 2 and 3, but with Ω k = 0.4 (closed universe * ). Be sure to keep the seed value the same as before. Include the label K-.4 in the two file names when they are saved. Ω K (curvature parameter) Age of universe Ω Λ (dark energy fraction) Ω m (matter fraction, dark+ ordinary) l value at spectrum peak 180 /l = angular scale of fluctuations Flat Universe Open Universe Closed Universe * More commonly, k denotes curvature. But Ω k ~ k.

3 6. Start up the ds9 software. File -> Open the fits file that you have labeled K.4. Click on zoom -> to fit then color -> rainbow. To adjust the color of your map so that it approximates the colors used by WMAP cosmologists, go to the menu Color -> Colormap Parameters and for Contrast enter 1.45985 and for Bias enter 0.54379 then click Apply. Close the Colormap Parameters menu. 7. Magenta is not part of the WMAP color scheme, so it must be removed. From the menu, select Edit -> Colorbar. On the colorbar at the bottom of the screen, clicking once at the left edge of the blue region should create a red patch. Drag the left edge of the red patch as far left as possible so that the magenta region is completely covered. Now double-click on the newly created red region to reveal a Color pop-up menu. Change Color from Red to Black then click OK. Question 3. Although the universe was extremely hot at its beginning 13.7 billion years ago, today its temperature is only 2.7 K ( 454.8 F). The WMAP project has observed tiny fluctuations in the temperature, however. Use the color bar below the map to determine the most common (not the largest) temperature fluctuation above 2.7 K, and the most common (not the smallest) temperature fluctuation below 2.7 K. Most common temp. fluctuation above 2.7 K = Most common temp. fluctuation below 2.7 K = 8. Go to File -> Save Image in either JPEG or PNG 24-bit formats. Don t forget to include K.4 in the file name. Do not close your image in ds9 because the same setting can be re-used. 9. File -> Open the fits file that you have labeled K0, and the K.0 image replaces the K.4 image with the color settings unchanged. Question 4. Use the color bar below the map to determine the most common (not the largest) temperature fluctuation above 2.7 K, and the most common (not the smallest) temperature fluctuation below 2.7 K. Most common temp. fluctuation above 2.7 K = Most common temp. fluctuation below 2.7 K = Save as in step 8. Again, do not close your image in ds9. 10. File -> Open the fits file that you have labeled K-.4.

4 Question 5. Use the color bar below the map to determine the most common (not the largest) temperature fluctuation above 2.7 K, and the most common (not the smallest) temperature fluctuation below 2.7 K. Most common temp. fluctuation above 2.7 K = Most common temp. fluctuation below 2.7 K = Save as in step 8. Question 6. Compare the theoretical maps for Ω k = 0.4 (open universe) and Ω k = 0 (flat universe). Which of the two has the smallest details? Question 7. Compare the theoretical maps for Ω k = 0.4 (closed universe) and Ω k = 0 (flat universe). Which of the two has the smallest details? Question 8. Which of your theoretical maps most closely matches the temperature fluctuations map of our actual universe observed by the WMAP project on the attached page? Question 9. Which one of your three power spectra graphs most closely matches the power spectra of our actual universe observed by the WMAP project on the attached page? Question 10. Do your answers to Questions 8 and 9 correspond to the same values of Ω k? If not consult with your instructor. Question 11. From the answers to the previous two questions, what kind of universe do we live in, open, flat, or closed? Question 12. To understand what the temperature fluctuations tell us about the curvature of the universe, record the l value for the maximum peak from each of the three power spectra graphs in the table above. Now calculate the angle associated with each l value.

5 Question 13. In the diagram below, the middle observer sees a spot in a flat universe. Notice the angle subtended by the spot. How does that angle compare to the angle (formed by the dashed lines) perceived by the observer in the open universe? In the closed universe? http://aether.lbl.gov/universe_shape.html Question 14. On the positive curvature and negative curvature diagrams above, draw the size of the spot that the observer actually sees. Do the relative sizes of the angles (Question 13) and spots in the diagram correspond to what you have recorded in the table for the angular scale of fluctuations, and to your answers to Questions 6 and 7 above?

WMAP satellite nine-year microwave sky, from http://wmap.gsfc.nasa.gov/media/121238/index.htm From Nine-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Final Maps and Results, Bennett, C.L., et al. 6