Added new tof test data

imap_processing/tests/ultra/unit/conftest.py

@@ -173,8 +173,8 @@ def decom_test_data(request, xtce_path):
 def events_fsw_comparison_theta_0():
     """FSW test data."""
     filename = (
-        "FM45_40P_Phi28p5_BeamCal_LinearScan_phi28.50_theta-0.00"
-        "_Ultra_Image_Raw_Event_20240207T102746_withFSWcalcs.csv"
+        "ultra45_raw_sc_ultrarawimg_withFSWcalcs_FM45_40P_Phi28p5_"
+        "BeamCal_LinearScan_phi2850_theta-000_20240207T102740.csv"
     )
     return (
         Path(sys.modules[__name__.split(".")[0]].__file__).parent

imap_processing/tests/ultra/unit/test_ultra_l1b_extended.py

@@ -7,6 +7,7 @@
 from imap_processing.ultra.l1b.ultra_l1b_extended import (
     StartType,
     StopType,
+    get_coincidence_positions,
     get_front_x_position,
     get_front_y_position,
     get_path_length,
@@ -30,12 +31,11 @@ def yf_fixture(de_dataset, events_fsw_comparison_theta_0):
 
 def test_get_front_x_position(
     de_dataset,
-    events_fsw_comparison_theta_0,
+    yf_fixture,
 ):
     """Tests get_front_x_position function."""
 
-    df = pd.read_csv(events_fsw_comparison_theta_0)
-    df_filt = df[df["StartType"] != -1]
+    df_filt, _, _ = yf_fixture
 
     xf = get_front_x_position(
         de_dataset["START_TYPE"].data,
@@ -50,6 +50,7 @@ def test_get_front_y_position(yf_fixture):
     df_filt, d, yf = yf_fixture
 
     assert yf == pytest.approx(df_filt["Yf"].astype("float"), abs=1e-5)
+    assert d == pytest.approx(df_filt["d"].astype("float"), abs=1e-5)
 
 
 def test_get_path_length(de_dataset, yf_fixture):
@@ -68,14 +69,13 @@ def test_get_path_length(de_dataset, yf_fixture):
 
 def test_get_ph_tof_and_back_positions(
     de_dataset,
-    events_fsw_comparison_theta_0,
+    yf_fixture,
 ):
     """Tests get_ph_tof_and_back_positions function."""
 
-    df = pd.read_csv(events_fsw_comparison_theta_0)
-    df_filt = df[df["StartType"] != -1]
+    df_filt, _, _ = yf_fixture
 
-    _, _, ph_xb, ph_yb = get_ph_tof_and_back_positions(
+    ph_tof, _, ph_xb, ph_yb = get_ph_tof_and_back_positions(
         de_dataset, df_filt.Xf.astype("float").values, "ultra45"
     )
 
@@ -87,6 +87,9 @@ def test_get_ph_tof_and_back_positions(
 
     np.testing.assert_array_equal(ph_xb, selected_rows["Xb"].astype("float"))
     np.testing.assert_array_equal(ph_yb, selected_rows["Yb"].astype("float"))
+    np.testing.assert_allclose(
+        ph_tof, selected_rows["TOF"].astype("float"), atol=1e-5, rtol=0
+    )
 
 
 def test_get_ssd_back_position_and_tof_offset(
@@ -127,3 +130,27 @@ def test_get_ssd_back_position_and_tof_offset(
     assert np.all(ssd_number_rt >= 0), "Values in ssd_number_rt out of range."
 
     assert np.all(ssd_number_rt <= 7), "Values in ssd_number_rt out of range."
+
+
+def test_get_coincidence_positions(de_dataset, yf_fixture):
+    """Tests get_coincidence_positions function."""
+    df_filt, _, _ = yf_fixture
+    # Get particle tof (t2).
+    _, t2, _, _ = get_ph_tof_and_back_positions(
+        de_dataset, df_filt.Xf.astype("float").values, "ultra45"
+    )
+
+    # Filter for stop type.
+    indices = np.nonzero(
+        np.isin(de_dataset["STOP_TYPE"], [StopType.Top.value, StopType.Bottom.value])
+    )[0]
+    de_filtered = de_dataset.isel(epoch=indices)
+    rows = df_filt.iloc[indices]
+
+    # Get coincidence position and eTOF.
+    etof, xc = get_coincidence_positions(de_filtered, t2, "ultra45")
+
+    np.testing.assert_allclose(xc, rows["Xc"].astype("float"), atol=1e-4, rtol=0)
+    np.testing.assert_allclose(
+        etof, rows["eTOF"].astype("float").values, rtol=0, atol=1e-06
+    )

imap_processing/ultra/l1b/lookup_utils.py

@@ -3,6 +3,7 @@
 import numpy as np
 import numpy.typing as npt
 import pandas as pd
+import xarray as xr
 
 from imap_processing import imap_module_directory
 
@@ -46,7 +47,7 @@ def get_y_adjust(dy_lut: np.ndarray) -> npt.NDArray:
     return _YADJUST_DF["dYAdj"].iloc[dy_lut].values
 
 
-def get_norm(dn: np.ndarray, key: str, file_label: str) -> npt.NDArray:
+def get_norm(dn: xr.DataArray, key: str, file_label: str) -> npt.NDArray:
     """
     Correct mismatches between the stop Time to Digital Converters (TDCs).
 

imap_processing/ultra/l1b/ultra_l1b_extended.py

@@ -39,6 +39,13 @@ class StopType(Enum):
     SSD: ClassVar[list[int]] = [8, 9, 10, 11, 12, 13, 14, 15]
 
 
+class CoinType(Enum):
+    """Coin Type: 1=Top, 2=Bottom."""
+
+    Top = 1
+    Bottom = 2
+
+
 def get_front_x_position(start_type: ndarray, start_position_tdc: ndarray) -> ndarray:
     """
     Calculate the front xf position.
@@ -161,7 +168,7 @@ def get_ph_tof_and_back_positions(
     Returns
     -------
     tof : np.array
-        Time of flight (tenths of a nanosecond).
+        Time of flight (nanoseconds).
     t2 : np.array
         Particle time of flight from start to stop (tenths of a nanosecond).
     xb : np.array
@@ -236,9 +243,6 @@ def get_ph_tof_and_back_positions(
         stop_type_bottom
     ] * get_image_params("XFTTOF")
 
-    # Multiply by 100 to get tenths of a nanosecond.
-    tof = tof * 100
-
     return tof, t2, xb, yb
 
 
@@ -315,3 +319,96 @@ def get_ssd_back_position_and_tof_offset(
         ] = get_image_params(f"TOFSSDRTOFF{i}")
 
     return yb, tof_offset, ssd_number
+
+
+def get_coincidence_positions(
+    de_dataset: xarray.Dataset, particle_tof: np.ndarray, sensor: str
+) -> tuple[np.ndarray, np.ndarray]:
+    """
+    Calculate coincidence positions.
+
+    Calculate time for electrons to travel back to
+    the coincidence anode (etof) and the x coincidence position (xc).
+
+    The tof measured by the coincidence anode consists of the particle
+    tof from start to stop, plus the time for the electrons to travel
+    back to the coincidence anode.
+
+    Further description is available on pages 34-35 of
+    IMAP-Ultra Flight Software Specification document
+    (7523-9009_Rev_-.pdf).
+
+    Parameters
+    ----------
+    de_dataset : xarray.Dataset
+        Data in xarray format.
+    particle_tof : np.ndarray
+        Particle time of flight (i.e. from start to stop)
+        (tenths of a nanosecond).
+    sensor : str
+        Sensor name.
+
+    Returns
+    -------
+    etof : np.ndarray
+        Time for the electrons to travel back to
+        coincidence anode (tenths of a nanosecond).
+    xc : np.ndarray
+        X coincidence position (hundredths of a millimeter).
+    """
+    index_top = np.nonzero(np.isin(de_dataset["COIN_TYPE"], CoinType.Top.value))[0]
+    de_top = de_dataset.isel(epoch=index_top)
+
+    index_bottom = np.nonzero(np.isin(de_dataset["COIN_TYPE"], CoinType.Bottom.value))[
+        0
+    ]
+    de_bottom = de_dataset.isel(epoch=index_bottom)
+
+    t1 = np.zeros(len(de_dataset["COIN_TYPE"]), dtype=np.float64)
+    t2 = np.zeros(len(de_dataset["COIN_TYPE"]), dtype=np.float64)
+
+    xc = np.zeros(len(de_dataset["COIN_TYPE"]), dtype=np.float64)
+    etof = np.zeros(len(de_dataset["COIN_TYPE"]), dtype=np.float64)
+
+    # Normalized TDCs
+    # For the stop anode, there are mismatches between the coincidence TDCs,
+    # i.e., CoinN and CoinS. They must be normalized via lookup tables.
+
+    # TpCoinNNorm Top
+    coin_n_norm_top = get_norm(de_top["COIN_NORTH_TDC"], "CoinN", sensor)
+    # TpCoinSNorm Top
+    coin_s_norm_top = get_norm(de_top["COIN_SOUTH_TDC"], "CoinS", sensor)
+
+    t1[index_top] = coin_n_norm_top + coin_s_norm_top  # /2 incorporated into scale
+    xc[index_top] = get_image_params("XCOINTPSC") * (
+        coin_s_norm_top - coin_n_norm_top
+    ) + get_image_params("XCOINTPOFF")  # millimeter
+    # Time for the electrons to travel back to coincidence anode.
+    t2[index_top] = get_image_params("ETOFSC") * t1[index_top] + get_image_params(
+        "ETOFTPOFF"
+    )
+
+    # Multiply by 10 to convert to tenths of a nanosecond.
+    etof[index_top] = t2[index_top] * 10 - particle_tof[index_top]
+
+    # TpCoinNNorm Bottom
+    coin_n_norm_bottom = get_norm(de_bottom["COIN_NORTH_TDC"], "CoinN", sensor)
+    # TpCoinSNorm Bottom
+    coin_s_norm_bottom = get_norm(de_bottom["COIN_SOUTH_TDC"], "CoinS", sensor)
+    t1[index_bottom] = (
+        coin_n_norm_bottom + coin_s_norm_bottom
+    )  # /2 incorporated into scale
+    xc[index_bottom] = get_image_params("XCOINBTSC") * (
+        coin_s_norm_bottom - coin_n_norm_bottom
+    ) + get_image_params("XCOINBTOFF")  # millimeter
+
+    # Time for the electrons to travel back to coincidence anode.
+    t2[index_bottom] = get_image_params("ETOFSC") * t1[index_bottom] + get_image_params(
+        "ETOFBTOFF"
+    )
+
+    # Multiply by 10 to convert to tenths of a nanosecond.
+    etof[index_bottom] = t2[index_bottom] * 10 - particle_tof[index_bottom]
+
+    # Convert to hundredths of a millimeter by multiplying times 100
+    return etof, xc * 100

imap_processing/ultra/lookup_tables/FM45_Startup1_ULTRA_IMGPARAMS_20240719.csv

@@ -1,2 +1,2 @@
 SHCOARSE,XFTSC,XFTLTOFF,XFTRTOFF,TOFSC,TOFTPOFF,TOFBTOFF,XFTTOF,XCOINTPSC,XCOINTPOFF,XCOINBTSC,XCOINBTOFF,ETOFSC,ETOFTPOFF,ETOFBTOFF,TOFDIFFTPMIN,TOFDIFFTPMAX,TOFDIFFBTMIN,TOFDIFFBTMAX,ETOFMIN,ETOFMAX,ETOFSLOPE1,ETOFOFF1,ETOFSLOPE2,ETOFOFF2,SPTPPHOFF,SPBTPHOFF,YBKSSD0,YBKSSD1,YBKSSD2,YBKSSD3,YBKSSD4,YBKSSD5,YBKSSD6,YBKSSD7,TOFSSDSC,TOFSSDLTOFF0,TOFSSDLTOFF1,TOFSSDLTOFF2,TOFSSDLTOFF3,TOFSSDLTOFF4,TOFSSDLTOFF5,TOFSSDLTOFF6,TOFSSDLTOFF7,TOFSSDRTOFF0,TOFSSDRTOFF1,TOFSSDRTOFF2,TOFSSDRTOFF3,TOFSSDRTOFF4,TOFSSDRTOFF5,TOFSSDRTOFF6,TOFSSDRTOFF7,TOFSSDTOTOFF,PATHSTEEPTHRESH,PATHMEDIUMTHRESH
-,0.172998047,49.3,48.25,0.5,-528,-525,0.001831055,0.067929688,41.75,0.067929688,-39.79492188,0.1,-44.5,-44.5,,,,,,,,,,,,,29.3,37.3,7.1,15.1,-15.1,-7.1,-37.3,-29.3,0.196484375,-6,-7.3,-3.8,-4.2,-3.8,-3.7,-6.3,-5,-5,-6.3,-3.7,-3.8,-4,-4.2,-7.3,-6,5.9,,
+,0.172998047,49.3,48.25,0.5,-528,-525,0.001831055,0.067929688,41.75,0.067929688,-40.75,0.1,-44.5,-44.5,,,,,,,,,,,,,29.3,37.3,7.1,15.1,-15.1,-7.1,-37.3,-29.3,0.196484375,-6,-7.3,-3.8,-4.2,-3.8,-3.7,-6.3,-5,-5,-6.3,-3.7,-3.8,-4,-4.2,-7.3,-6,5.9,,