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Table 2 Characteristics of the BDS PPP models

From: PPP models and performances from single- to quad-frequency BDS observations

Models

Signals

e1

e2

e3

e4

Ion.

Noise amplifications

SF1

B1I

1

0

0

0

1

1

SF2

B1I

1/2

0

0

0

0

1/4

SF3

B1I

1

0

0

0

1

1

DF1

B1I

1

0

0

0

1

1

B3I

0

1

0

0

1

1

DF2

B1I/B3I

2.944

− 1.944

0

0

0

3.528

DF3

B1I

1/2

0

0

0

0

1/4

B3I

1/2

0

0

0

0

1/4

B1I/B3I

2.944

− 1.944

0

0

0

3.528

DF4

B1I

1

0

0

0

1

1

B3I

0

1

0

0

1

1

TF1

B1I

1

0

0

0

1

1

B3I

0

1

0

0

1.514

1

B2a

0

0

1

0

1.761

1

TF2

B1I/B3I

2.944

− 1.944

0

0

0

3.528

B1I/B2a

2.314

0

− 1.314

0

0

2.662

TF3

B1I/B3I/B2a

2.343

− 0.089

− 1.254

0

0

2.659

B1I/B3I

2.944

− 1.944

0

0

0

3.528

TF4

B1I

1

0

0

0

1

1

B3I

0

1

0

0

1.514

1

B2a

0

0

1

0

1.761

1

QF1

B1I

1

0

0

0

1

1

B3I

0

1

0

0

1.514

1

B1C

0

0

1

0

0.982

1

B2a

0

0

0

1

1.761

1

QF2

B1I/B3I

2.944

− 1.944

0

0

0

3.528

B1C/B2a

0

0

2.261

− 1.261

0

2.588

QF3

B1I/B3I/B1C/B2a

1.171

− 0.336

1.224

− 1.058

0

2.025

B1I/B3I

2.944

− 1.944

0

0

0

3.528

QF4

B1I

1

0

0

0

1

1

B3I

0

1

0

0

1.514

1

B1C

0

0

1

0

0.982

1

B2a

0

0

0

1

1.761

1