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1 1 33 Years of Polar Aeronomy in Svalbard A review of scientific adventures north of 78º by Charles Deehr Prof. Emer. Phys. The Geophysical Institute University of Alaska Fairbanks

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Page 1: 33 Years of Polar Aeronomy in Svalbardkho.unis.no/doc/33_Years_of_Polar_Aeronomy_in_Svalbard.pdf · twilight) • The tilt of the geomagnetic field relative to the equatorial plane

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33 Years of Polar Aeronomy in Svalbard

A review of scientific adventures north of 78ºby

Charles DeehrProf. Emer. Phys.

The Geophysical InstituteUniversity of Alaska Fairbanks

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Magnetospheric CuspsMagnetosphericMagnetospheric CuspsCusps

• Magnetosp here has two cavities toward the sun.

• Concave singularity points

• Magnetosp here has two cavities toward the sun.

• Concave singularity points

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Magnetospheric CuspMagnetospheric Cusp

• Footpoint of cusp is near 75º magnetic latitude.

• Sun is >10º below horizon in shaded area during northern winter.

• Svalbard and Franz Josef Land only observatories

• Footpoint of cusp is near 75º magnetic latitude.

• Sun is >10º below horizon in shaded area during northern winter.

• Svalbard and Franz Josef Land only observatories

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Location of ObservatoriesLocation of Observatories

• Locations of outlying stations allowed some larger coverage.

• Ny Aalesund a major scientific station in geomag. meridian.

• Hopen and Hornsund secondary stations.

• Locations of outlying stations allowed some larger coverage.

• Ny Aalesund a major scientific station in geomag. meridian.

• Hopen and Hornsund secondary stations.

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Access to SvalbardAccess to Svalbard

• From 1596, the islands were accessible only by ship.

• Last ship out in Dec., first ship in in May.

• Daily commercial jet service established in 1975

• From 1596, the islands were accessible only by ship.

• Last ship out in Dec., first ship in in May.

• Daily commercial jet service established in 1975

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LongyearbyenLongyearbyen

• A coal mining town from 1914.• Now mainly tourist with hotels, etc.• A coal mining town from 1914.• Now mainly tourist with hotels, etc.

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Dayside Aurora from Svalbard 1970Dayside Aurora from Svalbard 1970• Establishing an Auroral Observatory at

Longyearbyen, October 1970 • Egeland, Omholt arrange UiO Physics Dept sponsor

hut construction and transport to Breinosa.

• Establishing an Auroral Observatory at Longyearbyen, October 1970

• Egeland, Omholt arrange UiO Physics Dept sponsor hut construction and transport to Breinosa.

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EISCAT on Breinosa 1996EISCAT on Breinosa 1996

• Hut on Breinosa in 1970 replaced by EISCAT• Northern Lights Station moved to valley (arrow)• Hut on Breinosa in 1970 replaced by EISCAT• Northern Lights Station moved to valley (arrow)

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Dayside Aurora from Svalbard 1978Dayside Aurora from Svalbard 1978• U of Tromsø, U of Oslo, U of Alaska, NSF establish

Nordlysstasjonen I Adventdalen, Summer 1978. • U of Tromsø, U of Oslo, U of Alaska, NSF establish

Nordlysstasjonen I Adventdalen, Summer 1978.

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Dayside Aurora from Svalbard 1978Dayside Aurora from Svalbard 1978

Multi-national Svalbard Auroral Expedition - 1978-79Multi-national Svalbard Auroral Expedition - 1978-79

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Dayside Observations Early 1980sDayside Observations Early 1980s

• Soviet stations at Barentsberg, Grumantbyen and Pyramiden

• Visits • Here is bust of Lenin

and a look-alike in Barentsberg.

• Soviet stations at Barentsberg, Grumantbyen and Pyramiden

• Visits • Here is bust of Lenin

and a look-alike in Barentsberg.

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Dayside Aurora from Svalbard 1978Dayside Aurora from Svalbard 1978

• Instruments outdoors led to stressful maintenance.• Instruments outdoors led to stressful maintenance.

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Dayside Aurora from Svalbard 1980Dayside Aurora from Svalbard 1980

• Polar bears outdoors led to stressful maintenance.• Polar bears outdoors led to stressful maintenance.

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Three Years at LYRThree Years at LYR

• Headlines in the local newspaper “Auroral researchers in Adventdalen for the third year in a row”

• Headlines in the local newspaper “Auroral researchers in Adventdalen for the third year in a row”

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Dayside Aurora from Svalbard - 1984Dayside Aurora from Svalbard - 1984

• Permanent station built 1984, expanded 1988.• Permanent station built 1984, expanded 1988.

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Dayside Aurora from Svalbard - 1984Dayside Aurora from Svalbard - 1984

• Calibration and observation in warmth and comfort.• Calibration and observation in warmth and comfort.

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Dayside Aurora from Svalbard - 1988Dayside Aurora from Svalbard - 1988• Permanent station expanded in 1988, used as command

center for rocket launches from SvalRak and Andoya. • Permanent station expanded in 1988, used as command

center for rocket launches from SvalRak and Andoya.

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Simultaneous from Svalbard & AlaskaSimultaneous from Svalbard & Alaska

• IMF Bz southward turning begins equatorward movement simultaneously on day and night side.

• There is aurora in the “Dayside Gap”

• A northward motion of the dayside aurora occurs within 15 min of all substorm onsets.

• IMF Bz southward turning begins equatorward movement simultaneously on day and night side.

• There is aurora in the “Dayside Gap”

• A northward motion of the dayside aurora occurs within 15 min of all substorm onsets.

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Auroral Emission SpectraAuroral Emission Spectra

Dayside auroral spectra were almost devoid of molecular bands, allowing new view of atomic emissions in the aurora. It was like a great red aurora every day for about an hour.

Dayside auroral spectra were almost devoid of molecular bands, allowing new view of atomic emissions in the aurora. It was like a great red aurora every day for about an hour.

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F-region Neutral and Ion WindsF-region Neutral and Ion Winds

• Roger Smith and students from Ireland used Fabry-Perot measurements of Doppler shifted atomic lines to measure winds.

• Roger Smith and students from Ireland used Fabry-Perot measurements of Doppler shifted atomic lines to measure winds.

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OH and O2 AirglowOH and O2 Airglow

• Polar airglow emissions from the 85 & 100 km altitude regions.

• Temperature measured from relative emission line intensities.

• Polar airglow emissions from the 85 & 100 km altitude regions.

• Temperature measured from relative emission line intensities.

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OH and O2 AirglowOH and O2 Airglow

• Polar airglow emissions from the 85 & 100 km altitude regions.

• Temperature measured from relative emission line intensities.

• Polar airglow emissions from the 85 & 100 km altitude regions.

• Temperature measured from relative emission line intensities.

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OH and O2 AirglowOH and O2 Airglow

• Stratospheric warmings are associated with mesospheric cooling.

• Cooling occurs simultaneously over polar region.

• Stratwarm is regional

• Stratospheric warmings are associated with mesospheric cooling.

• Cooling occurs simultaneously over polar region.

• Stratwarm is regional

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OH and O2 AirglowOH and O2 Airglow

• Stratospheric warmings are associated with mesospheric cooling.

• Cooling occurs simultaneously over polar region.

• Stratwarm is regional.• Note that small, warm

(-30º) region circulates into polar region and breaks up cold polar stratosphere.

• Stratospheric warmings are associated with mesospheric cooling.

• Cooling occurs simultaneously over polar region.

• Stratwarm is regional.• Note that small, warm

(-30º) region circulates into polar region and breaks up cold polar stratosphere.

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OH and O2 AirglowOH and O2 Airglow

• Large variations in mesopause temperature are correlated best with the zonal wind at 30hPa near 45º N lat.

• Large variations in mesopause temperature are correlated best with the zonal wind at 30hPa near 45º N lat.

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OH and O2 AirglowOH and O2 Airglow

• Large variations in mesopause temperature are correlated best with the zonal wind at 30hPa near 45º N lat.

• 20 year record shows little change in mesopause temperature at 78º N Lat.

• Large variations in mesopause temperature are correlated best with the zonal wind at 30hPa near 45º N lat.

• 20 year record shows little change in mesopause temperature at 78º N Lat.

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“SCIFER” Rocket Observations“SCIFER” Rocket Observations• Rocket borne

observations coordinated with ground-based optical and magnetic data.

• Launched from Andoya 06:24:48, January 25, 1995.

• Apogee 1452 km over Svalbard near 75º MLat. 10 MLT.

• Rocket borne observations coordinated with ground-based optical and magnetic data.

• Launched from Andoya 06:24:48, January 25, 1995.

• Apogee 1452 km over Svalbard near 75º MLat. 10 MLT.

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SCIFER TrajectorySCIFER Trajectory• Trajectory was

directly over Svalbard.

• 140 km magnetic conjugates below trajectory are linked to MSP along constant geomagnetic L shells.

• Trajectory was directly over Svalbard.

• 140 km magnetic conjugates below trajectory are linked to MSP along constant geomagnetic L shells.

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SCIFER Optical Auroral Observations

SCIFER Optical Auroral Observations

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SCIFER Energetic Electron FluxSCIFER Energetic Electron Flux• Objective of the

study is to identify the ionospheric signatures of the various particle populations.

• Objective of the study is to identify the ionospheric signatures of the various particle populations.

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Photoelectron Poleward BoundaryPhotoelectron Poleward Boundary• SCIFER flight at

1450 km over dayside aurora.

• Electron trapping boundary at 720 sec flight time.

• Magnetic zenith at LYR (L=15).

• Isotropic electron flux < 100 eV equatorward from boundary

• SCIFER flight at 1450 km over dayside aurora.

• Electron trapping boundary at 720 sec flight time.

• Magnetic zenith at LYR (L=15).

• Isotropic electron flux < 100 eV equatorward from boundary

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Predawn Enhancement 6300Å AirglowPredawn Enhancement 6300Å Airglow• Observations

from France by Barbier

• England by Roger Smith

• I. S. Radar Community

• Alaska and Oslo by C. Deehr

• Kiruna attempt with G. Gustavson

• Observations from France by Barbier

• England by Roger Smith

• I. S. Radar Community

• Alaska and Oslo by C. Deehr

• Kiruna attempt with G. Gustavson

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Magnetic Conjugate Photoelectrons

Magnetic Conjugate Photoelectrons

• This is a map of the extent of sunlit atmosphere during northern winter at 0200 UT. (astronomical twilight)

• The tilt of the geomagnetic field relative to the equatorial plane is such that the southern conjugate region is sunlit well before dawn over Europe.

• This is a map of the extent of sunlit atmosphere during northern winter at 0200 UT. (astronomical twilight)

• The tilt of the geomagnetic field relative to the equatorial plane is such that the southern conjugate region is sunlit well before dawn over Europe.

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Conjugate Photoelectrons from OsloConjugate Photoelectrons from Oslo

• Birefringent photometer from the roof of the Chemistry Building at University of Oslo.

• Increase in 6300 A airglow seen to coincide with the conjugate solar zenith angles 90-106 for L = 2.6 (SSW) and L = 5 (NNW).

• Birefringent photometer from the roof of the Chemistry Building at University of Oslo.

• Increase in 6300 A airglow seen to coincide with the conjugate solar zenith angles 90-106 for L = 2.6 (SSW) and L = 5 (NNW).

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Photoelectron Poleward BoundaryPhotoelectron Poleward Boundary• SCIFER flight at

1450 km over dayside aurora.

• Electron trapping boundary at 720 sec flight time.

• Magnetic zenith at LYR (L=15).

• Isotropic electron flux < 100 eV equatorward from boundary

• SCIFER flight at 1450 km over dayside aurora.

• Electron trapping boundary at 720 sec flight time.

• Magnetic zenith at LYR (L=15).

• Isotropic electron flux < 100 eV equatorward from boundary

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Photoelectron Poleward Boundary

Photoelectron Poleward Boundary

• Expected limit was L=4.

• Difficult to detect 100 to 200 R of 6300 Å emission near the auroral oval at L=5-6.

• SCIFER and CAPER rockets launched over the dayside aurora (L=6 to 30).

• Expected limit was L=4.

• Difficult to detect 100 to 200 R of 6300 Å emission near the auroral oval at L=5-6.

• SCIFER and CAPER rockets launched over the dayside aurora (L=6 to 30).

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Photoelectron Energy SpectrumPhotoelectron Energy Spectrum• Theoretical

photoelectron spectrum by G. Khasanov shows detail due to structure in solar EUV flux.

• SCIFER observations indicate photoelectrons.

• Theoretical photoelectron spectrum by G. Khasanov shows detail due to structure in solar EUV flux.

• SCIFER observations indicate photoelectrons.

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Local or Conjugate Photoelectrons?

Local or Conjugate Photoelectrons?

• Earliest local production of photoelectrons is dependent on solar EUV flux.

• Proxy for EUV is 10.7 cm flux.

• Solar EUV during SCIFER and CAPER below that required to produce local photoelectons at 106° sza.

• Earliest local production of photoelectrons is dependent on solar EUV flux.

• Proxy for EUV is 10.7 cm flux.

• Solar EUV during SCIFER and CAPER below that required to produce local photoelectons at 106° sza.

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SCIFER Energetic Electron FluxSCIFER Energetic Electron Flux• Objective of the

study is to identify the ionospheric signatures of the various particle populations.

• 0-80 eV are photoelectrons from conjugate region.

• Objective of the study is to identify the ionospheric signatures of the various particle populations.

• 0-80 eV are photoelectrons from conjugate region.

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Southern Sky Brightness Pulsations

Southern Sky Brightness Pulsations

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Particle Energy Flux & All-Sky Camera

Particle Energy Flux & All-Sky Camera

• Total correlation coeff. = 0.6

• Variations with periods of magnetic pulsations Pc 1, 3, 5 are shown.

• There are two pulses that are unrelated.

• Pc 5 (180 s) and Pc 3 (43 s) correlate with 1- 5 keV electron flux.

• Total correlation coeff. = 0.6

• Variations with periods of magnetic pulsations Pc 1, 3, 5 are shown.

• There are two pulses that are unrelated.

• Pc 5 (180 s) and Pc 3 (43 s) correlate with 1- 5 keV electron flux.

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SCIFER Energetic Electron FluxSCIFER Energetic Electron Flux• Objective of the

study is to identify the ionospheric signatures of the various particle populations.

• 0-80 eV (<700 sec) are conjugate photoelectrons.

• 1-5 keV (<700sec) are wave/particle interaction pulsations.

• Objective of the study is to identify the ionospheric signatures of the various particle populations.

• 0-80 eV (<700 sec) are conjugate photoelectrons.

• 1-5 keV (<700sec) are wave/particle interaction pulsations.

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Energy-dispersed BurstsEnergy-dispersed Bursts• All-sky camera brightness

pulses • Energy dispersed from 1

to >15 keV. • Dispersion indicates loss

cone injection near equator.

• Bounce times = n x 1/2 length of field line.

• Energy flux = 0.2 ergs/cm2sec, implying most flux > 15 keV.

• All-sky camera brightness pulses

• Energy dispersed from 1 to >15 keV.

• Dispersion indicates loss cone injection near equator.

• Bounce times = n x 1/2 length of field line.

• Energy flux = 0.2 ergs/cm2sec, implying most flux > 15 keV.

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Particle Energy Flux & All-Sky Camera

Particle Energy Flux & All-Sky Camera

• Sky brightness in the equatorward sky compared with simultaneous observations of energetic electron precipitation in the same region.

• Broad-band all-sky camera intensity pulses correlate with energy-dispersed bursts in the energetic electrons.

• Correlation coeff. = 0.7.• There is no magnetometer

data to confirm the relationship to Pc 1 pulsations

• Sky brightness in the equatorward sky compared with simultaneous observations of energetic electron precipitation in the same region.

• Broad-band all-sky camera intensity pulses correlate with energy-dispersed bursts in the energetic electrons.

• Correlation coeff. = 0.7.• There is no magnetometer

data to confirm the relationship to Pc 1 pulsations

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SCIFER Energetic Electron FluxSCIFER Energetic Electron Flux• Comparison of

optical and particle data yields origin of particles.

• 0-80 eV are conjugate photoelectrons.

• 1-5 keV are wave/particle interaction along closed field line.

• >5 keV energy dispersed bursts from wave/particle interaction equator.

• Comparison of optical and particle data yields origin of particles.

• 0-80 eV are conjugate photoelectrons.

• 1-5 keV are wave/particle interaction along closed field line.

• >5 keV energy dispersed bursts from wave/particle interaction equator.

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Poleward Discrete ArcsPoleward Discrete Arcs

• Inverted V particle signature over discrete arcs.

• Peak E >1 keV visible as arc on TV (~0.5 ergs/cm2sec).

• Inverted V particle signature over discrete arcs.

• Peak E >1 keV visible as arc on TV (~0.5 ergs/cm2sec).

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Magnetospheric BoundariesMagnetospheric Boundaries• Discrete aurora

poleward of trapping boundary.

• Wave/particle and merging processes produce pulsating aurora inside trapping boundary.

• Discrete aurora poleward of trapping boundary.

• Wave/particle and merging processes produce pulsating aurora inside trapping boundary.

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Geomagnetic Disturbance Signatures

Geomagnetic Disturbance Signatures

• There were two pulses of 1-5 keV electrons during the flight.

• They corresponded to increase in brightness and Magnetic Convection Vortices.

• There were two pulses of 1-5 keV electrons during the flight.

• They corresponded to increase in brightness and Magnetic Convection Vortices.

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Geomagnetic Disturbance Signatures

Geomagnetic Disturbance Signatures

• The Pc 5 magnetic pulsations, the optical pulsations and the TCV are produced by the 1-5 keV electron pulses inside the trapping boundary.

• The Pc 5 magnetic pulsations, the optical pulsations and the TCV are produced by the 1-5 keV electron pulses inside the trapping boundary.

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Convection VelocityConvection Velocity

• Convection sunward inside trapping boundary.

• Anti-sunward poleward.• Speed minimum inside

arcs.

• Convection sunward inside trapping boundary.

• Anti-sunward poleward.• Speed minimum inside

arcs.

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Relationship to Convection PatternRelationship to Convection Pattern• Midmorning.• IMF Bz < 0.• 40 keV trapping

boundary coincident with convection reversal.

• Midmorning.• IMF Bz < 0.• 40 keV trapping

boundary coincident with convection reversal.

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Observed Convection PatternObserved Convection Pattern

• IMF Bz < 0.• IMF By > 0.• PMAFs near 40.• Ion dispersion

observed.

• IMF Bz < 0.• IMF By > 0.• PMAFs near 40.• Ion dispersion

observed.

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Hypothetical Convection PatternHypothetical Convection Pattern

• IMF Bz < 0.• 5 different types

of auroral forms associated with convection pattern.

• LYR moves under the convection pattern S of the station shown here.

• IMF Bz < 0.• 5 different types

of auroral forms associated with convection pattern.

• LYR moves under the convection pattern S of the station shown here.

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The Dayside GapThe Dayside Gap• Gap in dayside

aurora is shown to be diminished 5577 A emission.

• 6300 A shows a slight gap also.

• 6300 A/5577A ratio inversely proportional to incoming electron energy.

• Minimum energy around magnetic noon.

• Gap in dayside aurora is shown to be diminished 5577 A emission.

• 6300 A shows a slight gap also.

• 6300 A/5577A ratio inversely proportional to incoming electron energy.

• Minimum energy around magnetic noon.

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IMF Effect on Dayside GapIMF Effect on Dayside Gap• 6300

A/5577A ratio inversely proportional to incoming electron energy.

• Minimum energy in afternoon for By>0, in the morning for By<0

• 6300 A/5577A ratio inversely proportional to incoming electron energy.

• Minimum energy in afternoon for By>0, in the morning for By<0

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Hypothetical Convection PatternHypothetical Convection Pattern

• IMF Bz < 0.• 5 different types

of auroral forms associated with convection pattern.

• Type 1a in the convection throat is less energetic than type 1b in the merging line

• IMF Bz < 0.• 5 different types

of auroral forms associated with convection pattern.

• Type 1a in the convection throat is less energetic than type 1b in the merging line

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CAPER TrajectoryCAPER Trajectory

• Flew West of planned trajectory over LYR.

• As with SCIFER, the 140 km conjugate position was linked to the MSP scan along constant L shells for comparison.

• Flew West of planned trajectory over LYR.

• As with SCIFER, the 140 km conjugate position was linked to the MSP scan along constant L shells for comparison.

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CAPER Energetic Electron FluxCAPER Energetic Electron Flux• CAPER similar to

SCIFER. • Except

– discrete forms both equatorward and poleward of TB.

– Conjugate photoelectrons end short of TB.

• CAPER similar to SCIFER.

• Except – discrete forms both

equatorward and poleward of TB.

– Conjugate photoelectrons end short of TB.

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CAPER Meridian PhotometerCAPER Meridian Photometer

• Discrete forms on poleward and equatorward side of TB.• Pulsations on equatorward side of TB.• Discrete forms on poleward and equatorward side of TB.• Pulsations on equatorward side of TB.

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IMF B Variations & Optical Aurora

IMF B Variations & Optical Aurora

• IMF Bz near zero. IMF By positive.

• Two discrete arc regions separated by trapping boundary.

• Northward turning Bz produces forms in both regions at 0640 UT.

• Southward turning near 0700 UT produces form poleward of TB.

• IMF Bz near zero. IMF By positive.

• Two discrete arc regions separated by trapping boundary.

• Northward turning Bz produces forms in both regions at 0640 UT.

• Southward turning near 0700 UT produces form poleward of TB.

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CAPER Ion and ElectronsCAPER Ion and Electrons• Origin of auroral forms

in the two regions is found in the particle data.

• Ion velocity dispersion indicates convection in two directions from the TB.

• Origin of auroral forms in the two regions is found in the particle data.

• Ion velocity dispersion indicates convection in two directions from the TB.

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Conjugate Photoelectrons to L=15

Conjugate Photoelectrons to L=15

• Non-local photoelectrons on both flights in dayside aurora.

• Photoelectron transport from conjugate region observed to L=15

• Field lines equatorward of discrete aurora are closed and dipolar.

• Non-local photoelectrons on both flights in dayside aurora.

• Photoelectron transport from conjugate region observed to L=15

• Field lines equatorward of discrete aurora are closed and dipolar.

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Dayside MergingDayside Merging

• SCIFER IMF Bz < 0 • CAPER IMF Bz > 0• Newly open field lines • Newly closed and opened• SCIFER IMF Bz < 0 • CAPER IMF Bz > 0• Newly open field lines • Newly closed and opened

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CAPER Convection VelocityCAPER Convection Velocity• Sunward convection

equatorward of TB. • Anti-sunward

convection poleward of TB.

• Fastest speed between arcs.

• CAPER showed broader convection reversal region than SCIFER.

• Sunward convection equatorward of TB.

• Anti-sunward convection poleward of TB.

• Fastest speed between arcs.

• CAPER showed broader convection reversal region than SCIFER.

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“CAPER” Rocket Observations“CAPER” Rocket Observations

• Motion of convection is E-W along the auroral forms.

• Equatorward forms show sunward convection motion.

• Poleward forms show anti- sunward convection motion.

• Motion of convection is E-W along the auroral forms.

• Equatorward forms show sunward convection motion.

• Poleward forms show anti- sunward convection motion.

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Pressure Pulse AuroraPressure Pulse Aurora

• Speed of pulse along the magnetopause is consistent with 15 km/sec advance of aurora.

• Speed of pulse along the magnetopause is consistent with 15 km/sec advance of aurora.

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Solar Wind Shock Arrival, Oct 21, 02

Solar Wind Shock Arrival, Oct 21, 02

• Large area of luminosity equatorward of oval at 17:00:26 UT• Two minutes later moved to 10am and 2pm.• Reached midnight in 8 minutes.

• Large area of luminosity equatorward of oval at 17:00:26 UT• Two minutes later moved to 10am and 2pm.• Reached midnight in 8 minutes.

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Solar Wind Shock Dec. 10, 1997Solar Wind Shock Dec. 10, 1997

• WIND satellite observed shock in the solar wind at 04:30 UT.

• WIND satellite observed shock in the solar wind at 04:30 UT.

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Dayside Pressure Pulse AuroraDayside Pressure Pulse Aurora

• Initial aurora from pressure pulse is equatorward of TB. • Initial aurora from pressure pulse is equatorward of TB.

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Pressure Pulse AuroraPressure Pulse Aurora• Polar UVI observations of

pressure pulse aurora . • Red dots show ground

stations: – LYR at 0900 MLT observed

diffuse electron aurora. – PKR, Ft Smith, Gillam

observed H emissions in the evening MLT.

• We conclude that this aurora results from disturbance of gradient drift particles inside the TB by the pressure pulse.

• Polar UVI observations of pressure pulse aurora .

• Red dots show ground stations:– LYR at 0900 MLT observed

diffuse electron aurora.– PKR, Ft Smith, Gillam

observed H emissions in the evening MLT.

• We conclude that this aurora results from disturbance of gradient drift particles inside the TB by the pressure pulse.

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Dayside Magnetospheric Boundaries

Dayside Magnetospheric Boundaries

• Aurora from Merging• Aurora from Pressure Pulses• Aurora from K/H

• Aurora from Merging• Aurora from Pressure Pulses• Aurora from K/H