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GPS RO for atmospheric studiesGPS RO for atmospheric studies
Panagiotis Vergados
Dept of Physics and Astronomy Dept of Physics and Astronomy
OutlineOutline
Objectives Introduction Description of the techniques Fresnel diffraction theory Radio-holography Back-propagation theory Atmospheric parameters retrieval Remarks Work in progress amp future work
ObjectivesObjectives
Develop knowledge and expertise in GPS RO studies Review and understand currently used methods and models Choose and improve the method which gives the best vertical resolution
of refractive index profiles retrieve atmospheric parameters (such as temperature and water vapour)
from refractive index profiles
Introduction (1)Introduction (1)
There is an increased interest in high vertical and horizontal resolutionhigh vertical and horizontal resolution observations and global ndash scale coverageglobal ndash scale coverage of temperature and water vapour
Yunck et al (1988) suggested that the Global Positioning SystemGlobal Positioning System (GPS)(GPS) be used to make Radio Occultation (RO) observations of the Earthrsquos atmosphere
The era for GPS RO observations of the Earthrsquos atmosphere began with the GPS Meteorology (GPSMET) experiment on April 3April 3rdrd 1995 1995 [Ware et al 1996 Kursinski et al 1996 1997]
Introduction (2)Introduction (2)
Radio occultation (RO) experiment geometry
The RO techniqueRO technique
Bending angle α
Impact parameter a
Spacecraft distance D
Introduction (3)Introduction (3)
Standard method to calculate refractivity profiles Able Inversion TransformAble Inversion Transform of bending angle profilesof bending angle profiles
HOW do you calculate bending angle profilesHOW do you calculate bending angle profiles
Through measurements of the Doppler-shifted phase of the received electric field and observation geometry of the experiment
ProblemsProblems Diffraction and Multi-path effect
FACT 1 strong gradients of water vapourstrong gradients of water vapour in the lower troposphere cause diffraction and multi-pathdiffraction and multi-path which limit the vertical resolution of the measurements
FACT 2 First-order ionospheric correction not sufficient (L1 and L2 follow two different paths)
Various methods have been introduced in order to overcome these limitations
Fresnel diffraction theory Radio-holography Back-propagation theory
Description of the techniques (1)Description of the techniques (1)
ApproximationsApproximations
Thin screen Thin screen [[Melbourne et al 1994 Mortensen and Hoeg 1998] and] and
Spherical symmetrySpherical symmetry
Fresnel Diffraction (1)Fresnel Diffraction (1)
AdvantagesAdvantages
Introduction of a weighting functionIntroduction of a weighting function
Vertical resolution is not diffraction limited
Multi-path effects can be reduced
Fresnel Diffraction (contrsquod)Fresnel Diffraction (contrsquod)
Vertical temperature difference profiles
a) =52o N
b) 70o N (Mortensen et al 1998)
Error estimates
plusmn 2oC (between 5 and 25 km)
gt 2oC (below 5 km)
Vertical resolution
Few hundreds of m to 1 km5
10
15
20
a b
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
OutlineOutline
Objectives Introduction Description of the techniques Fresnel diffraction theory Radio-holography Back-propagation theory Atmospheric parameters retrieval Remarks Work in progress amp future work
ObjectivesObjectives
Develop knowledge and expertise in GPS RO studies Review and understand currently used methods and models Choose and improve the method which gives the best vertical resolution
of refractive index profiles retrieve atmospheric parameters (such as temperature and water vapour)
from refractive index profiles
Introduction (1)Introduction (1)
There is an increased interest in high vertical and horizontal resolutionhigh vertical and horizontal resolution observations and global ndash scale coverageglobal ndash scale coverage of temperature and water vapour
Yunck et al (1988) suggested that the Global Positioning SystemGlobal Positioning System (GPS)(GPS) be used to make Radio Occultation (RO) observations of the Earthrsquos atmosphere
The era for GPS RO observations of the Earthrsquos atmosphere began with the GPS Meteorology (GPSMET) experiment on April 3April 3rdrd 1995 1995 [Ware et al 1996 Kursinski et al 1996 1997]
Introduction (2)Introduction (2)
Radio occultation (RO) experiment geometry
The RO techniqueRO technique
Bending angle α
Impact parameter a
Spacecraft distance D
Introduction (3)Introduction (3)
Standard method to calculate refractivity profiles Able Inversion TransformAble Inversion Transform of bending angle profilesof bending angle profiles
HOW do you calculate bending angle profilesHOW do you calculate bending angle profiles
Through measurements of the Doppler-shifted phase of the received electric field and observation geometry of the experiment
ProblemsProblems Diffraction and Multi-path effect
FACT 1 strong gradients of water vapourstrong gradients of water vapour in the lower troposphere cause diffraction and multi-pathdiffraction and multi-path which limit the vertical resolution of the measurements
FACT 2 First-order ionospheric correction not sufficient (L1 and L2 follow two different paths)
Various methods have been introduced in order to overcome these limitations
Fresnel diffraction theory Radio-holography Back-propagation theory
Description of the techniques (1)Description of the techniques (1)
ApproximationsApproximations
Thin screen Thin screen [[Melbourne et al 1994 Mortensen and Hoeg 1998] and] and
Spherical symmetrySpherical symmetry
Fresnel Diffraction (1)Fresnel Diffraction (1)
AdvantagesAdvantages
Introduction of a weighting functionIntroduction of a weighting function
Vertical resolution is not diffraction limited
Multi-path effects can be reduced
Fresnel Diffraction (contrsquod)Fresnel Diffraction (contrsquod)
Vertical temperature difference profiles
a) =52o N
b) 70o N (Mortensen et al 1998)
Error estimates
plusmn 2oC (between 5 and 25 km)
gt 2oC (below 5 km)
Vertical resolution
Few hundreds of m to 1 km5
10
15
20
a b
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
ObjectivesObjectives
Develop knowledge and expertise in GPS RO studies Review and understand currently used methods and models Choose and improve the method which gives the best vertical resolution
of refractive index profiles retrieve atmospheric parameters (such as temperature and water vapour)
from refractive index profiles
Introduction (1)Introduction (1)
There is an increased interest in high vertical and horizontal resolutionhigh vertical and horizontal resolution observations and global ndash scale coverageglobal ndash scale coverage of temperature and water vapour
Yunck et al (1988) suggested that the Global Positioning SystemGlobal Positioning System (GPS)(GPS) be used to make Radio Occultation (RO) observations of the Earthrsquos atmosphere
The era for GPS RO observations of the Earthrsquos atmosphere began with the GPS Meteorology (GPSMET) experiment on April 3April 3rdrd 1995 1995 [Ware et al 1996 Kursinski et al 1996 1997]
Introduction (2)Introduction (2)
Radio occultation (RO) experiment geometry
The RO techniqueRO technique
Bending angle α
Impact parameter a
Spacecraft distance D
Introduction (3)Introduction (3)
Standard method to calculate refractivity profiles Able Inversion TransformAble Inversion Transform of bending angle profilesof bending angle profiles
HOW do you calculate bending angle profilesHOW do you calculate bending angle profiles
Through measurements of the Doppler-shifted phase of the received electric field and observation geometry of the experiment
ProblemsProblems Diffraction and Multi-path effect
FACT 1 strong gradients of water vapourstrong gradients of water vapour in the lower troposphere cause diffraction and multi-pathdiffraction and multi-path which limit the vertical resolution of the measurements
FACT 2 First-order ionospheric correction not sufficient (L1 and L2 follow two different paths)
Various methods have been introduced in order to overcome these limitations
Fresnel diffraction theory Radio-holography Back-propagation theory
Description of the techniques (1)Description of the techniques (1)
ApproximationsApproximations
Thin screen Thin screen [[Melbourne et al 1994 Mortensen and Hoeg 1998] and] and
Spherical symmetrySpherical symmetry
Fresnel Diffraction (1)Fresnel Diffraction (1)
AdvantagesAdvantages
Introduction of a weighting functionIntroduction of a weighting function
Vertical resolution is not diffraction limited
Multi-path effects can be reduced
Fresnel Diffraction (contrsquod)Fresnel Diffraction (contrsquod)
Vertical temperature difference profiles
a) =52o N
b) 70o N (Mortensen et al 1998)
Error estimates
plusmn 2oC (between 5 and 25 km)
gt 2oC (below 5 km)
Vertical resolution
Few hundreds of m to 1 km5
10
15
20
a b
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Introduction (1)Introduction (1)
There is an increased interest in high vertical and horizontal resolutionhigh vertical and horizontal resolution observations and global ndash scale coverageglobal ndash scale coverage of temperature and water vapour
Yunck et al (1988) suggested that the Global Positioning SystemGlobal Positioning System (GPS)(GPS) be used to make Radio Occultation (RO) observations of the Earthrsquos atmosphere
The era for GPS RO observations of the Earthrsquos atmosphere began with the GPS Meteorology (GPSMET) experiment on April 3April 3rdrd 1995 1995 [Ware et al 1996 Kursinski et al 1996 1997]
Introduction (2)Introduction (2)
Radio occultation (RO) experiment geometry
The RO techniqueRO technique
Bending angle α
Impact parameter a
Spacecraft distance D
Introduction (3)Introduction (3)
Standard method to calculate refractivity profiles Able Inversion TransformAble Inversion Transform of bending angle profilesof bending angle profiles
HOW do you calculate bending angle profilesHOW do you calculate bending angle profiles
Through measurements of the Doppler-shifted phase of the received electric field and observation geometry of the experiment
ProblemsProblems Diffraction and Multi-path effect
FACT 1 strong gradients of water vapourstrong gradients of water vapour in the lower troposphere cause diffraction and multi-pathdiffraction and multi-path which limit the vertical resolution of the measurements
FACT 2 First-order ionospheric correction not sufficient (L1 and L2 follow two different paths)
Various methods have been introduced in order to overcome these limitations
Fresnel diffraction theory Radio-holography Back-propagation theory
Description of the techniques (1)Description of the techniques (1)
ApproximationsApproximations
Thin screen Thin screen [[Melbourne et al 1994 Mortensen and Hoeg 1998] and] and
Spherical symmetrySpherical symmetry
Fresnel Diffraction (1)Fresnel Diffraction (1)
AdvantagesAdvantages
Introduction of a weighting functionIntroduction of a weighting function
Vertical resolution is not diffraction limited
Multi-path effects can be reduced
Fresnel Diffraction (contrsquod)Fresnel Diffraction (contrsquod)
Vertical temperature difference profiles
a) =52o N
b) 70o N (Mortensen et al 1998)
Error estimates
plusmn 2oC (between 5 and 25 km)
gt 2oC (below 5 km)
Vertical resolution
Few hundreds of m to 1 km5
10
15
20
a b
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Introduction (2)Introduction (2)
Radio occultation (RO) experiment geometry
The RO techniqueRO technique
Bending angle α
Impact parameter a
Spacecraft distance D
Introduction (3)Introduction (3)
Standard method to calculate refractivity profiles Able Inversion TransformAble Inversion Transform of bending angle profilesof bending angle profiles
HOW do you calculate bending angle profilesHOW do you calculate bending angle profiles
Through measurements of the Doppler-shifted phase of the received electric field and observation geometry of the experiment
ProblemsProblems Diffraction and Multi-path effect
FACT 1 strong gradients of water vapourstrong gradients of water vapour in the lower troposphere cause diffraction and multi-pathdiffraction and multi-path which limit the vertical resolution of the measurements
FACT 2 First-order ionospheric correction not sufficient (L1 and L2 follow two different paths)
Various methods have been introduced in order to overcome these limitations
Fresnel diffraction theory Radio-holography Back-propagation theory
Description of the techniques (1)Description of the techniques (1)
ApproximationsApproximations
Thin screen Thin screen [[Melbourne et al 1994 Mortensen and Hoeg 1998] and] and
Spherical symmetrySpherical symmetry
Fresnel Diffraction (1)Fresnel Diffraction (1)
AdvantagesAdvantages
Introduction of a weighting functionIntroduction of a weighting function
Vertical resolution is not diffraction limited
Multi-path effects can be reduced
Fresnel Diffraction (contrsquod)Fresnel Diffraction (contrsquod)
Vertical temperature difference profiles
a) =52o N
b) 70o N (Mortensen et al 1998)
Error estimates
plusmn 2oC (between 5 and 25 km)
gt 2oC (below 5 km)
Vertical resolution
Few hundreds of m to 1 km5
10
15
20
a b
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Introduction (3)Introduction (3)
Standard method to calculate refractivity profiles Able Inversion TransformAble Inversion Transform of bending angle profilesof bending angle profiles
HOW do you calculate bending angle profilesHOW do you calculate bending angle profiles
Through measurements of the Doppler-shifted phase of the received electric field and observation geometry of the experiment
ProblemsProblems Diffraction and Multi-path effect
FACT 1 strong gradients of water vapourstrong gradients of water vapour in the lower troposphere cause diffraction and multi-pathdiffraction and multi-path which limit the vertical resolution of the measurements
FACT 2 First-order ionospheric correction not sufficient (L1 and L2 follow two different paths)
Various methods have been introduced in order to overcome these limitations
Fresnel diffraction theory Radio-holography Back-propagation theory
Description of the techniques (1)Description of the techniques (1)
ApproximationsApproximations
Thin screen Thin screen [[Melbourne et al 1994 Mortensen and Hoeg 1998] and] and
Spherical symmetrySpherical symmetry
Fresnel Diffraction (1)Fresnel Diffraction (1)
AdvantagesAdvantages
Introduction of a weighting functionIntroduction of a weighting function
Vertical resolution is not diffraction limited
Multi-path effects can be reduced
Fresnel Diffraction (contrsquod)Fresnel Diffraction (contrsquod)
Vertical temperature difference profiles
a) =52o N
b) 70o N (Mortensen et al 1998)
Error estimates
plusmn 2oC (between 5 and 25 km)
gt 2oC (below 5 km)
Vertical resolution
Few hundreds of m to 1 km5
10
15
20
a b
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
FACT 1 strong gradients of water vapourstrong gradients of water vapour in the lower troposphere cause diffraction and multi-pathdiffraction and multi-path which limit the vertical resolution of the measurements
FACT 2 First-order ionospheric correction not sufficient (L1 and L2 follow two different paths)
Various methods have been introduced in order to overcome these limitations
Fresnel diffraction theory Radio-holography Back-propagation theory
Description of the techniques (1)Description of the techniques (1)
ApproximationsApproximations
Thin screen Thin screen [[Melbourne et al 1994 Mortensen and Hoeg 1998] and] and
Spherical symmetrySpherical symmetry
Fresnel Diffraction (1)Fresnel Diffraction (1)
AdvantagesAdvantages
Introduction of a weighting functionIntroduction of a weighting function
Vertical resolution is not diffraction limited
Multi-path effects can be reduced
Fresnel Diffraction (contrsquod)Fresnel Diffraction (contrsquod)
Vertical temperature difference profiles
a) =52o N
b) 70o N (Mortensen et al 1998)
Error estimates
plusmn 2oC (between 5 and 25 km)
gt 2oC (below 5 km)
Vertical resolution
Few hundreds of m to 1 km5
10
15
20
a b
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
ApproximationsApproximations
Thin screen Thin screen [[Melbourne et al 1994 Mortensen and Hoeg 1998] and] and
Spherical symmetrySpherical symmetry
Fresnel Diffraction (1)Fresnel Diffraction (1)
AdvantagesAdvantages
Introduction of a weighting functionIntroduction of a weighting function
Vertical resolution is not diffraction limited
Multi-path effects can be reduced
Fresnel Diffraction (contrsquod)Fresnel Diffraction (contrsquod)
Vertical temperature difference profiles
a) =52o N
b) 70o N (Mortensen et al 1998)
Error estimates
plusmn 2oC (between 5 and 25 km)
gt 2oC (below 5 km)
Vertical resolution
Few hundreds of m to 1 km5
10
15
20
a b
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Fresnel Diffraction (contrsquod)Fresnel Diffraction (contrsquod)
Vertical temperature difference profiles
a) =52o N
b) 70o N (Mortensen et al 1998)
Error estimates
plusmn 2oC (between 5 and 25 km)
gt 2oC (below 5 km)
Vertical resolution
Few hundreds of m to 1 km5
10
15
20
a b
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Radio-holography (1)Radio-holography (1)
ApproximationsApproximations
Account for a reference electric field Em(t) = exp(iφ(t))
Construct a radio-hologram ΔE(t) = E(t) Em (t)
Assume the radio-hologram is consisted of complex sine-waves
Governing equationsGoverning equations m (the bending angle)
ppm + p(the impact parameter)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Radio-holography (contrsquod)Radio-holography (contrsquod)
Vertical temperature difference profiles a) 28o b) 36o and c) 48oN (Hocke et al 1999)
Error Estimates
plusmn 17 ndash 33 oK (between 5 and 25 km)
plusmn 5 oK (below 5 km)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Back propagation (1)Back propagation (1)
ApproximationsApproximations
Multiple Phase Screen (MPS) [Karayel et al 1997]
Spherically symmetric atmosphere
AdvantagesAdvantages
Diffraction and multi-path effects are mostly removed
Much better vertical resolution below the sub-Fresnel scale
Back-propagation of the electric field rays to an auxiliary plane
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Back-propagation (contrsquod)Back-propagation (contrsquod)
Vertical temperature profile of a terrestrial atmosphere(Karayel et al 1997)
Error estimates
range 02 oK to 2 oK
Vertical resolution
Around 250 m (terrestrial atmosphere)
Around 40 m (Martian atmosphere)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Atmospheric parametersAtmospheric parameters
After the refractive index profile has been constructed atmospheric parameters can be calculated through
N = a1∙P T + a2∙Pw T2
where P and Pw are the atmospheric and water vapour pressure T is the temperature at the respective pressure level and a1 and a2 are constants
Known Refractive index profile and either P or T
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
RemarksRemarks
Fresnel Diffraction Theory Radio-holography and Back-propagation remove mostly the diffraction and multi-path effects
The vertical resolution achieved from all three methods ranges approximately from a few hundred meters to 1 km
The back-propagation method is capable of achieving vertical resolution at sub-Fresnel scales (lt 250 m)
The error estimates of the retrieved temperature profiles with the back-propagation method range between 02 and 2 K and of the refractive index profile between 410-6 and 1410-5
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
Work in progress and future workWork in progress and future work
Second and third order ionospheric correction in the calculation of bending angle profiles
Abel inversion investigation and possible improvement
Modification andor development of software for ionospheric correction and Abel inversion transform
Investigation of the non-spherical symmetry and how it affects the refractive index profile
Investigation of other possible methods and development of an improved model for the retrieval of atmospheric parameters from refractive index profiles (eg 1D-VAR method)
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