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Today in History – 30 September

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Today in History - 30 September

1207

Rumi, famous Muslim Sufi poet, was born.

1687

Aurangzeb acquired the famous Golconda fort near Hyderabad from the Qutub Shahi Sultan Tana Shah due to the treachery of his General Panni.

1791

Mozart’s opera The Magic Flute is performed for the first time in Vienna

1908

Ram Dhari Singh Dinkar, famous Hindi novelist, was born.

1911

Italy declares war on Turkey over control of Tripoli.

1918

Bulgaria pulls out of World War I.

1949

The Berlin Airlift is officially halted after 277,264 flights.

1954

The first atomic-powered submarine, the Nautilus, was commissioned in Groton, Connecticut.

1954

NATO nations agree to arm and admit West Germany.

1963

The USSR openly louded Indian view on Kashmir issue. This was against Pakistan’s motives.

1972

Pakistani troops shell into the Indian zone of Kashmir.

1981

Pakistan Commando soldiers release 66 hostages in Lahore from five Khalistan hijackers and activists of the Dal Khalsa International.

1989

INS Shalki, India’s first indigenously built submarine, launched in Bombay.

1992

Laurie Baker wins Rs. 25 lakh UN World Habitat award.

1996

Centre gives its consent to Tamil Nadu government’s decision to rename Madras as Chennai.

1997

24th Stock Exchange of India set up at Trivandrum.

1999

India successfully test-fired its multi-target surface-to-air missile ‘Akash’.

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Information Paradox

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Table of Contents

  1. Introduction
  2. Classical Black Holes and No-Hair Theorem
  3. Quantum Fields and Hawking Radiation
  4. Thermal Nature of Hawking Radiation
  5. Statement of the Paradox
  6. Unitarity in Quantum Mechanics
  7. Black Hole Evaporation
  8. Information Loss Hypothesis
  9. Conflicts with Quantum Theory
  10. The Page Curve and Entropy Evolution
  11. Entanglement Structure of Hawking Radiation
  12. The Monogamy of Entanglement
  13. The AMPS Firewall Argument
  14. Black Hole Complementarity
  15. The Role of Quantum Gravity
  16. String Theory Perspective
  17. The AdS/CFT Resolution
  18. Holography and Boundary Unitarity
  19. Quantum Extremal Surfaces and Replica Wormholes
  20. Page Curve from Semiclassical Gravity
  21. Remnants Hypothesis
  22. Information Retrieval from Radiation
  23. Experimental Outlook and Analog Models
  24. Implications for Spacetime and Causality
  25. Conclusion

1. Introduction

The information paradox challenges the foundations of physics by suggesting that black holes might violate the principle of unitarity in quantum mechanics. The paradox arises when we try to reconcile quantum field theory with black hole thermodynamics and general relativity.


2. Classical Black Holes and No-Hair Theorem

Classically, black holes are defined by only a few parameters: mass, charge, and angular momentum. This is known as the no-hair theorem. All other information is lost beyond the event horizon, which presents no problem in classical general relativity.


3. Quantum Fields and Hawking Radiation

Hawking showed that black holes emit radiation due to quantum effects near the event horizon. This Hawking radiation appears thermal and leads to gradual black hole evaporation.


4. Thermal Nature of Hawking Radiation

Hawking radiation carries no information about the infalling matter. It appears completely thermal and uncorrelated, raising questions about what happens to the information that formed the black hole.


5. Statement of the Paradox

If a black hole completely evaporates, and the radiation is thermal, then the process is non-unitary — violating a fundamental axiom of quantum mechanics. This leads to the black hole information paradox.


6. Unitarity in Quantum Mechanics

Unitarity implies that the evolution of a closed quantum system preserves information and probabilities. A pure quantum state should evolve into another pure state — not a mixed state.


7. Black Hole Evaporation

The evaporation time of a black hole is:

\[
t_{\text{evap}} \sim \frac{G^2 M^3}{\hbar c^4}
\]

As the black hole evaporates, entropy in the radiation grows, seemingly transforming a pure state into a mixed state.


8. Information Loss Hypothesis

One early resolution proposed that information is lost when the black hole evaporates. However, this would require modifying the standard rules of quantum mechanics and violates unitarity.


9. Conflicts with Quantum Theory

Information loss would:

  • Prevent time-reversal symmetry
  • Introduce unpredictability
  • Break superposition and linearity
  • Challenge the consistency of quantum field theory

10. The Page Curve and Entropy Evolution

Don Page predicted that the entropy of Hawking radiation should first increase, then decrease — forming a Page curve consistent with unitary evolution.


11. Entanglement Structure of Hawking Radiation

Each emitted Hawking quantum is entangled with a partner falling into the black hole. Over time, the number of outside entangled pairs grows, leading to rising radiation entropy.


12. The Monogamy of Entanglement

Quantum mechanics forbids a particle from being maximally entangled with two systems. After the Page time, outgoing radiation cannot be entangled both with earlier radiation and interior modes — creating a paradox.


13. The AMPS Firewall Argument

Almheiri, Marolf, Polchinski, and Sully proposed that to resolve the paradox, entanglement must break at the horizon, creating a firewall — a high-energy region that destroys infalling observers, violating general relativity’s equivalence principle.


14. Black Hole Complementarity

Suggests no single observer sees a contradiction:

  • Outside observer sees information in radiation
  • Infalling observer sees smooth spacetime

Avoids paradox by observer-dependent reality — though it’s hard to reconcile globally.


15. The Role of Quantum Gravity

A full theory of quantum gravity may resolve the paradox by modifying spacetime at the Planck scale, introducing nonlocality, or providing new degrees of freedom.


16. String Theory Perspective

In string theory, black holes have microstates — specific brane configurations. For certain extremal black holes, counting these states reproduces the Bekenstein–Hawking entropy, suggesting no information loss.


17. The AdS/CFT Resolution

In the AdS/CFT correspondence, black hole evaporation in AdS is dual to unitary evolution in a conformal field theory. This implies that information is preserved, at least in these settings.


18. Holography and Boundary Unitarity

The holographic principle posits that the entire bulk spacetime, including black holes, is encoded on a boundary theory. If the boundary is unitary, then so must be the bulk.


19. Quantum Extremal Surfaces and Replica Wormholes

Recent work using quantum extremal surfaces and replica wormholes has shown how to recover the Page curve from semiclassical gravity, suggesting unitary evaporation with late-time information recovery.


20. Page Curve from Semiclassical Gravity

These methods compute entanglement entropy directly and reproduce the rise-and-fall behavior predicted by Page — consistent with information preservation.


21. Remnants Hypothesis

Proposes that stable Planck-scale remnants store information after evaporation. However, this raises issues with infinite degeneracy and observable consequences.


22. Information Retrieval from Radiation

Another possibility is that Hawking radiation carries subtle quantum correlations encoding the original information, but these are too subtle to be captured by semiclassical approximations.


23. Experimental Outlook and Analog Models

While direct detection is infeasible, analog black holes (e.g., in fluids, BECs) may help test aspects of Hawking radiation and information loss in controlled environments.


24. Implications for Spacetime and Causality

The information paradox challenges core principles:

  • Locality
  • Causality
  • Horizon smoothness

Resolving it may require a radical reformulation of spacetime and quantum information.


25. Conclusion

The black hole information paradox sits at the intersection of gravity, quantum mechanics, and thermodynamics. It has led to profound insights in holography, entropy, and quantum gravity. While full resolution is still evolving, recent advances — especially from AdS/CFT and replica wormholes — point toward unitarity and subtle information recovery mechanisms. The paradox continues to be a guiding puzzle in the quest for quantum gravity.


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Today in History – 29 September

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Today in History - 29 September

1708

British East India Company and New East India company merged.

1755

Robert Lord Clive founded the British empire in India.

1789

Congress votes to create a U.S. army.

1836

Chamber of Commerce and Industry was established in Madras.

1850

Mormon leader Brigham Young is named the first governor of the Utah Territory.

1907

Labour MP James Keir Hardie accuses UK of running India ‘like the Czar runs Russia’.

1914

German cruiser Emden shells Madras.

1914

Japanese vessel ‘Kamagata Maru’ reached Baj Baj near Calcutta from Vancouver carrying Indian revolutionaries.

1932

A five-day work week is established for General Motors workers.

1939

Germany and the Soviet Union reach an agreement on the division of Poland.

1942

The British police shot Matangini Hazra, a 72-year old woman of Tamluk town in Midnapur district, when she was leading the flag at Tamluk in August movement procession.

1951

Michelle Bachelet, first woman president of Chile (2006-10).

1959

Arati Saha successfully swam the English Channel. She was the first Asian lady to achieve the feat.

1962

Canada launches its first satellite, Alouette 1.

1970

Union Carbide India Ltd in Bombay was commissioned Reclamation Plant Sewage Water of India for commercial use.

1971

Oman joins the Arab League.

1977

India and Bangladesh signed settlement for distributing Ganga river water.

1979

John Paul II becomes the first pope ever to visit Ireland.

1981

Delhi-Srinagar Indian Airlines Boeing 737 flight was diverted to Lahore, Pakistan by five Khalistan activists of the Dal Khalsa International. On board there were 117 passengers out of which 66 were freed on arrival in Lahore.

1988

Nobel Peace Prize for U.N. Peace-Keeping Forces.

1990

The YF-22, later named F-22 Raptor, flies for the first time.

1991

Ustad Yunus Hussain Khan, famous singer of ‘Agra Gharana’, passed away.

1993

National Human Rights Commission set up.

1994

Cable Television Regulation Ordinance issued.

1998

ISRO successfully launches its largest sounding rocket, Rohini (RH-560 mk, 11 total payload, 127 kg).

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Hawking Radiation

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Table of Contents

  1. Introduction
  2. Black Holes in Classical Physics
  3. Thermodynamic Analogy
  4. Quantum Fields in Curved Spacetime
  5. Event Horizon and Particle Production
  6. Heuristic Derivation of Hawking Radiation
  7. Bogoliubov Transformations and Particle Creation
  8. Hawking’s Original Calculation
  9. Temperature of a Black Hole
  10. Blackbody Spectrum and Thermal Nature
  11. Energy Loss and Black Hole Evaporation
  12. Life Cycle of a Black Hole
  13. Backreaction and Semi-Classical Gravity
  14. Hawking Radiation in Different Black Hole Types
  15. Greybody Factors and Spectrum Modification
  16. Analogue Systems: Acoustic Black Holes
  17. Hawking Radiation in de Sitter and AdS Space
  18. Information Loss Paradox
  19. Entanglement Across the Horizon
  20. Page Time and the Page Curve
  21. Firewall Debate and Alternatives
  22. Resolution Proposals: Unitarity and Remnants
  23. Recent Developments: Replica Wormholes
  24. Experimental Prospects
  25. Conclusion

1. Introduction

Hawking radiation is the quantum mechanical process by which black holes emit thermal radiation. Predicted by Stephen Hawking in 1974, it fundamentally changed our understanding of black holes by linking quantum mechanics, gravity, and thermodynamics.


2. Black Holes in Classical Physics

Classically, black holes are perfect absorbers — no information or matter can escape from within the event horizon. This led to paradoxes when considering entropy and energy balance.


3. Thermodynamic Analogy

The laws of black hole mechanics closely resemble those of thermodynamics. Bekenstein proposed that black holes have entropy proportional to their horizon area, setting the stage for Hawking’s work.


4. Quantum Fields in Curved Spacetime

Hawking’s analysis uses quantum field theory in curved spacetime, where particles are defined with respect to observers’ time coordinates. The event horizon creates a fundamental mismatch in definitions.


5. Event Horizon and Particle Production

Near the horizon, quantum fluctuations can result in virtual particle–antiparticle pairs. One particle falls into the black hole, the other escapes, appearing as real radiation to a distant observer.


6. Heuristic Derivation of Hawking Radiation

Imagine vacuum fluctuations near the horizon:

  • One particle falls in with negative energy (relative to infinity)
  • The other escapes, conserving total energy

The black hole loses mass — interpreted as thermal radiation emission.


7. Bogoliubov Transformations and Particle Creation

More rigorously, one compares in- and out-modes of the quantum field using Bogoliubov transformations. This reveals a non-zero number of outgoing particles seen by an asymptotic observer.


8. Hawking’s Original Calculation

Hawking computed the particle flux using semiclassical gravity:

  • Background: collapsing star forming a black hole
  • Field: massless scalar field in this background
  • Result: thermal spectrum with temperature

9. Temperature of a Black Hole

For a Schwarzschild black hole:

\[
T_H = \frac{\hbar c^3}{8\pi G M k_B}
\]

This implies the black hole emits like a blackbody with this temperature.


10. Blackbody Spectrum and Thermal Nature

Hawking radiation has a nearly Planckian spectrum. However, it is not exactly thermal due to greybody factors — frequency-dependent transmission coefficients.


11. Energy Loss and Black Hole Evaporation

As it radiates, the black hole loses mass:

\[
\frac{dM}{dt} \propto – \frac{1}{M^2}
\]

Eventually, it may evaporate completely unless new physics halts the process.


12. Life Cycle of a Black Hole

Stages:

  • Formation
  • Quasi-stable phase
  • Accelerated evaporation (as \( M \to 0 \))
  • Final fate: unknown — singularity? remnant? bounce?

13. Backreaction and Semi-Classical Gravity

Hawking’s calculation neglects backreaction (effect of radiation on geometry). Including it remains a major open problem in quantum gravity.


14. Hawking Radiation in Different Black Hole Types

  • Reissner–Nordström and Kerr black holes have modified temperatures
  • Extremal black holes (e.g., maximal charge or spin) have \( T_H = 0 \)

15. Greybody Factors and Spectrum Modification

Emission is affected by the black hole’s potential barrier. Greybody factors reduce high- and low-energy emission compared to ideal blackbody spectrum.


16. Analogue Systems: Acoustic Black Holes

“Sonically” trapped phonons in Bose–Einstein condensates or fluids exhibit analog Hawking radiation, potentially observable in laboratory experiments.


17. Hawking Radiation in de Sitter and AdS Space

Similar mechanisms apply to:

  • de Sitter space: cosmological horizons radiate
  • Anti-de Sitter (AdS): modified boundary behavior, related via AdS/CFT

18. Information Loss Paradox

If Hawking radiation is purely thermal, no information about the initial state escapes — violating unitarity of quantum mechanics. This is the black hole information paradox.


19. Entanglement Across the Horizon

Early and late radiation becomes entangled. After the Page time, continued evaporation leads to a contradiction if one assumes unitarity and local quantum field theory.


20. Page Time and the Page Curve

Predicted by Don Page:

  • Entropy of radiation rises, peaks at Page time, then declines
  • Suggests that information is gradually encoded in the radiation

21. Firewall Debate and Alternatives

If information is preserved, entanglement must be broken — implying a firewall at the horizon. This contradicts general relativity and the equivalence principle.


22. Resolution Proposals: Unitarity and Remnants

Proposals to resolve the paradox:

  • Information leaks through subtle correlations
  • Remnants store remaining information
  • Holography and AdS/CFT suggest unitary evolution

23. Recent Developments: Replica Wormholes

Using techniques from quantum gravity and holography, replica wormholes allow statistical computation of entropy consistent with unitarity and the Page curve.


24. Experimental Prospects

Hawking radiation is far too faint to detect from astrophysical black holes. Analog models and gravitational wave observations offer indirect avenues.


25. Conclusion

Hawking radiation connects quantum theory, thermodynamics, and gravity in a profound way. It reveals that black holes are not eternal, and poses deep questions about the fate of information. As theoretical and observational tools improve, Hawking radiation continues to shape our understanding of spacetime, quantum fields, and the ultimate laws of physics.


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Today in History – 28 September

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Today in History - 28 September

Today in History - 28 September

855

The Emperor Lothar dies in Gaul, and his kingdom is divided between his three sons.

1238

James of Aragon retakes Valencia, Spain, from the Arabs.

1827

A few mountain battery trains flourished and kept the Indian component alive as part of the Royal artillery. Recently, it has been established that 8 Company Bombay Artillery survived axing and is now 5 (Bombay) Mountain Battery. This day is now celebrated as the Raising Day of the Regiment of Artillery.

1837

Bahadur Shah-II ascended the throne and became the emperor of Delhi at the age of 62 following the death of his father Akbar Shah-II.

1912

W.C. Handy’s “Memphis Blues” is published.

1924

In penance for riots, Gandhi, on hunger strike in Delhi, proclaimed he would break his fast only at death.

1929

Lata Mangeshkar, great playback singer, was born.

1940

Pundit Sunder Lal Sharma, freedom fighter and social reformer, passed away. He was also known as “”The Chhattisgarh Gandhi”.

1958

France ratifies a new constitution.

1965

India-Pakistan hostility erupts into a war

1985

The first Indian Army expedition, sailing around the world in a small 37 feet fibre glass yacht named “”Trishna””, sailed off from Bombay.

2008

SpaceX launches the first private spacecraft, Falcon 1.

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