diff --git a/src/config.json b/src/config.json
index 19ebc43..080de22 100644
--- a/src/config.json
+++ b/src/config.json
@@ -1,34 +1,36 @@
 {
   "simulation": {
-    "num_walker": 5000,
+    "num_walker": 20,
     "seed": null
   },
   "molecule": {
     "delta": 161e3,
-    "eta": 0.0
+    "eta": 0.1
   },
   "correlation_times": {
-    "distribution": "LogGaussian",
+    "distribution": "DeltaDistribution",
     "tau": {
-      "start": 1e-4,
-      "stop": 1e-8,
-      "steps": 9,
-      "is_log": true
-    },
-    "sigma": {
-      "list": [0.5, 1, 2]
+      "list": [1e2, 1e0]
     }
   },
   "motion": {
-    "model": "TetrahedralJump"
+    "model": "RandomJump"
   },
   "spectrum": {
     "dwell_time": 1e-6,
     "num_points": 4096,
     "t_echo": {
-      "list": [5e-6, 10e-6, 20e-6, 40e-6, 60e-6, 100e-6]
+      "list": [
+        5e-6,
+        10e-6,
+        20e-6,
+        40e-6,
+        60e-6,
+        100e-6
+      ]
     },
-    "line_broadening": 2e3
+    "line_broadening": 4e3,
+    "t_pulse": 2e-6
   },
   "stimulated_echo": {
     "t_evo": {
diff --git a/src/config_ste.json b/src/config_ste.json
deleted file mode 100644
index befdd8b..0000000
--- a/src/config_ste.json
+++ /dev/null
@@ -1,30 +0,0 @@
-{
-  "simulation": {
-    "num_walker": 20000,
-    "seed": null
-  },
-  "molecule": {
-    "delta": 161e3,
-    "eta": 0.0
-  },
-  "correlation_times": {
-    "distribution": "DeltaDistribution",
-    "tau": 1e-2
-  },
-  "motion": {
-    "model": "RandomJump"
-  },
-  "stimulated_echo": {
-    "t_evo": {
-      "start": 1e-6,
-      "stop": 40e-6,
-      "steps": 80
-    },
-    "t_mix": {
-      "start": 1e-5,
-      "stop": 1e0,
-      "steps": 21,
-      "is_log": true
-    }
-  }
-}
\ No newline at end of file
diff --git a/src/rwsims/distributions.py b/src/rwsims/distributions.py
index 1490039..8752d78 100644
--- a/src/rwsims/distributions.py
+++ b/src/rwsims/distributions.py
@@ -12,7 +12,11 @@ class BaseDistribution(ABC):
         self._tau = tau
         self._rng = rng
 
-        self._tau_jump = tau
+        self.tau_jump = tau
+
+    @property
+    def name(self) -> str:
+        return self.__class__.__name__
 
     @abstractmethod
     def __repr__(self):
@@ -28,16 +32,16 @@ class BaseDistribution(ABC):
         pass
 
     def wait(self, size: int = 1) -> ArrayLike:
-        return self._rng.exponential(self._tau_jump, size=size)
+        return self._rng.exponential(self.tau_jump, size=size)
 
 
 class DeltaDistribution(BaseDistribution):
 
     def __repr__(self):
-        return f'No distribution(tau={self._tau})'
+        return f'Delta Distribution (tau={self._tau})'
 
     def start(self):
-        self._tau_jump = self._tau
+        self.tau_jump = self._tau
 
     @property
     def mean_tau(self):
@@ -54,7 +58,7 @@ class LogGaussianDistribution(BaseDistribution):
         return f'Log-Gaussian(tau={self._tau}, sigma={self._sigma})'
 
     def start(self):
-        self._tau_jump = self._rng.lognormal(np.log(self._tau), self._sigma)
+        self.tau_jump = self._rng.lognormal(np.log(self._tau), self._sigma)
 
     @property
     def mean_tau(self):
diff --git a/src/rwsims/functions.py b/src/rwsims/functions.py
new file mode 100644
index 0000000..0d33bbf
--- /dev/null
+++ b/src/rwsims/functions.py
@@ -0,0 +1,22 @@
+from __future__ import annotations
+
+import numpy as np
+from numpy.typing import ArrayLike
+
+from distributions import BaseDistribution
+from motions import BaseMotion
+
+
+def ste(x, a, f_infty, tau, beta):
+    return a*((1-f_infty) * np.exp(-(x/tau)**beta) + f_infty)
+
+
+def pulse_attn(freq: ArrayLike, t_pulse: float) -> ArrayLike:
+    # cf. Schmitt-Rohr/Spieß eq. 2.126; omega_1 * t_p = pi/2
+    pi_half_squared = np.pi**2 / 4
+    omega = 2 * np.pi * freq
+
+    numerator = np.sin(np.sqrt(pi_half_squared + omega**2 * t_pulse**2 / 2))
+    denominator = np.sqrt(pi_half_squared + omega**2 * t_pulse**2 / 4)
+
+    return np.pi * numerator/denominator / 2
\ No newline at end of file
diff --git a/src/rwsims/helper.py b/src/rwsims/helper.py
deleted file mode 100644
index 8f7fb1f..0000000
--- a/src/rwsims/helper.py
+++ /dev/null
@@ -1,65 +0,0 @@
-from __future__ import annotations
-
-import numpy as np
-from numpy.typing import ArrayLike
-from numpy.random import Generator
-
-
-def xyz_to_spherical(x_in: float, y_in: float, z_in: float) -> tuple[float, float, float]:
-    r = np.linalg.norm([x_in, y_in, z_in])
-    theta = np.arccos(z_in)
-    phi = np.arctan2(y_in, x_in)
-
-    return r, theta, phi
-
-
-def spherical_to_xyz(r: float, theta: float, phi: float) -> tuple[float, float, float]:
-    sin_theta = np.sin(theta)
-    return r*np.cos(phi)*sin_theta, r*np.sin(phi)*sin_theta, r*np.cos(theta)
-
-
-def get_rotation_matrix(vec_in: np.ndarray, vec_out: np.ndarray):
-    rotation = np.eye(3)
-
-    # rotation by angle around given axis
-    cos_angle = np.dot(vec_in, vec_out)
-
-    # check for parallel / anti-parallel vectors
-    if cos_angle == 1:
-        return rotation
-    elif cos_angle == -1:
-        return -rotation
-
-    else:
-        axis = np.cross(vec_in, vec_out)
-        scale = np.linalg.norm(axis)
-        axis /= scale
-        sin_angle = scale / np.linalg.norm(vec_in) / np.linalg.norm(vec_out)
-
-        v_cross = np.array([
-            [0,       -axis[2], axis[1]],
-            [axis[2], 0,        -axis[0]],
-            [-axis[1], axis[0], 0],
-        ])
-
-        rotation += sin_angle * v_cross
-        rotation += (1-cos_angle) * v_cross @ v_cross
-
-        return rotation
-
-
-def omega_q(delta: float, eta: float, theta: ArrayLike, phi: ArrayLike) -> ArrayLike:
-    cos_theta = np.cos(theta)
-    sin_theta = np.sin(theta)
-    return np.pi * delta * (3 * cos_theta**2 - 1 + eta * sin_theta**2 * np.cos(2*phi))
-
-
-def draw_orientation(rng: Generator, size: int | None = None) -> tuple[ArrayLike, ArrayLike]:
-    if size is not None:
-        z_theta, z_phi = rng.random((2, size))
-    else:
-        z_theta, z_phi = rng.random(2)
-    theta = np.arccos(1 - 2 * z_theta)
-    phi = 2 * np.pi * z_phi
-
-    return theta, phi
diff --git a/src/rwsims/motions.py b/src/rwsims/motions.py
index 6e55591..de2644d 100644
--- a/src/rwsims/motions.py
+++ b/src/rwsims/motions.py
@@ -6,8 +6,6 @@ import numpy as np
 from numpy.random import Generator
 from numpy.typing import ArrayLike
 
-from .helper import xyz_to_spherical, spherical_to_xyz, omega_q, draw_orientation, get_rotation_matrix
-
 
 class BaseMotion(ABC):
     def __init__(self, delta: float, eta: float, rng: Generator):
@@ -20,6 +18,10 @@ class BaseMotion(ABC):
     def __repr__(self):
         pass
 
+    @property
+    def name(self) -> str:
+        return self.__class__.__name__
+
     def start(self):
         pass
 
@@ -66,11 +68,11 @@ class TetrahedralJump(BaseMotion):
         ])
 
         # orientation in lab system
-        theta0, phi0 = draw_orientation(self._rng)
+        cos_theta0, phi0 = draw_orientation(self._rng)
 
         rot = get_rotation_matrix(
             corners[0],
-            np.array(spherical_to_xyz(1., theta0, phi0)),
+            np.array(spherical_to_xyz(1., np.arccos(cos_theta0), phi0)),
         )
         orientations = np.zeros(4)
         for i in range(4):
@@ -90,3 +92,66 @@ class TetrahedralJump(BaseMotion):
         return self._orientation[jumps]
 
 
+# Helper functions
+
+def xyz_to_spherical(x_in: float, y_in: float, z_in: float) -> tuple[float, float, float]:
+    r = np.linalg.norm([x_in, y_in, z_in])
+    theta = np.arccos(z_in)
+    phi = np.arctan2(y_in, x_in)
+
+    return r, theta, phi
+
+
+def spherical_to_xyz(r: float, theta: float, phi: float) -> tuple[float, float, float]:
+    sin_theta = np.sin(theta)
+    return r*np.cos(phi)*sin_theta, r*np.sin(phi)*sin_theta, r*np.cos(theta)
+
+
+def get_rotation_matrix(vec_in: np.ndarray, vec_out: np.ndarray):
+    rotation = np.eye(3)
+
+    # rotation by angle around given axis
+    cos_angle = np.dot(vec_in, vec_out)
+
+    # check for parallel / anti-parallel vectors
+    if cos_angle == 1:
+        return rotation
+    elif cos_angle == -1:
+        return -rotation
+
+    else:
+        axis = np.cross(vec_in, vec_out)
+        scale = np.linalg.norm(axis)
+        axis /= scale
+        sin_angle = scale / np.linalg.norm(vec_in) / np.linalg.norm(vec_out)
+
+        v_cross = np.array([
+            [0,       -axis[2], axis[1]],
+            [axis[2], 0,        -axis[0]],
+            [-axis[1], axis[0], 0],
+        ])
+
+        rotation += sin_angle * v_cross
+        rotation += (1-cos_angle) * v_cross @ v_cross
+
+        return rotation
+
+
+def omega_q(delta: float, eta: float, cos_theta: ArrayLike, phi: ArrayLike) -> ArrayLike:
+    # sin_theta = np.sin(cos_theta)
+    # cos_theta = np.cos(cos_theta)
+    sin_theta_sq = 1 - cos_theta**2
+    return np.pi * delta * (3 * cos_theta**2 - 1 + eta * sin_theta_sq * np.cos(2*phi))
+
+
+def draw_orientation(rng: Generator, size: int | None = None) -> tuple[ArrayLike, ArrayLike]:
+    if size is not None:
+        z_theta, z_phi = rng.random((2, size))
+    else:
+        z_theta, z_phi = rng.random(2)
+    cos_theta = 1 - 2 * z_theta
+    phi = 2 * np.pi * z_phi
+
+    return cos_theta, phi
+
+
diff --git a/src/rwsims/parameter.py b/src/rwsims/parameter.py
index 637029e..762f6de 100644
--- a/src/rwsims/parameter.py
+++ b/src/rwsims/parameter.py
@@ -6,7 +6,9 @@ from math import prod
 from typing import Any
 
 import numpy as np
+from numpy._typing import ArrayLike
 
+from functions import pulse_attn
 from .distributions import BaseDistribution
 from .motions import BaseMotion
 
@@ -27,6 +29,9 @@ class SimParameter:
     num_walker: int
     t_max: float
 
+    def totext(self) -> str:
+        return f'num_traj={self.num_walker}\nseed={self.seed}'
+
 
 @dataclass
 class MoleculeParameter:
@@ -36,8 +41,8 @@ class MoleculeParameter:
 
 @dataclass
 class StimEchoParameter:
-    t_evo: np.ndarray
-    t_mix: np.ndarray
+    t_evo: ArrayLike
+    t_mix: ArrayLike
     t_echo: float
     t_max: float = field(init=False)
 
@@ -49,16 +54,28 @@ class StimEchoParameter:
 class SpectrumParameter:
     dwell_time: float
     num_points: int
-    t_echo: np.ndarray
-    t_acq: np.ndarray = field(init=False)
-    t_max: float = field(init=False)
+    t_echo: ArrayLike
     lb: float
-    dampening: np.ndarray = field(init=False)
+    t_pulse: float
+    t_acq: ArrayLike = field(init=False)
+    freq: ArrayLike = field(init=False)
+    t_max: float = field(init=False)
+    dampening: ArrayLike = field(init=False)
+    pulse_attn: ArrayLike = field(init=False)
 
     def __post_init__(self):
         self.t_acq = np.arange(self.num_points) * self.dwell_time
         self.dampening = np.exp(-self.lb * self.t_acq)
         self.t_max = np.max(self.t_acq) + 2 * np.max(self.t_echo)
+        self.freq = np.fft.fftshift(np.fft.fftfreq(self.num_points, self.dwell_time))
+        self.pulse_attn = pulse_attn(self.freq, self.t_pulse)
+
+    def totext(self) -> str:
+        return (f'dwell_time{self.dwell_time}\n'
+                f'num_points={self.num_points}\n'
+                f't_echo={self.t_echo}\n'
+                f'lb={self.lb}\n'
+                f't_pulse={self.t_pulse}')
 
 
 @dataclass
@@ -115,3 +132,14 @@ class Parameter:
     dist: DistParameter
     motion: MotionParameter
     molecule: MoleculeParameter
+
+    def totext(self, sim: bool = True, spec: bool = True) -> str:
+        text = []
+        if sim:
+            text.append(self.sim.totext())
+
+        if spec:
+            text.append(self.spec.totext())
+
+        return '\n'.join(text)
+
diff --git a/src/rwsims/parsing.py b/src/rwsims/parsing.py
index a2cc9bf..3121af4 100644
--- a/src/rwsims/parsing.py
+++ b/src/rwsims/parsing.py
@@ -66,7 +66,8 @@ def _parse_spectrum(params: dict[str, Any] | None) -> SpectrumParameter | None:
         num_points=params['num_points'],
         dwell_time=params['dwell_time'],
         t_echo=_make_times(params['t_echo']),
-        lb=params['line_broadening']
+        lb=params.get('line_broadening', 0),
+        t_pulse=params.get('t_pulse', 0)
     )
 
     return spec
diff --git a/src/rwsims/sims.py b/src/rwsims/sims.py
index 3bd19a6..c486872 100644
--- a/src/rwsims/sims.py
+++ b/src/rwsims/sims.py
@@ -1,13 +1,15 @@
 from __future__ import annotations
 
-from time import time
+from time import perf_counter
 
 import numpy as np
 from numpy.random import Generator
+from datetime import datetime
 from scipy.interpolate import interp1d
 import matplotlib.pyplot as plt
 from scipy.optimize import curve_fit
 
+from .functions import ste
 from .parameter import Parameter
 from .distributions import BaseDistribution
 from .motions import BaseMotion
@@ -31,32 +33,31 @@ def run_ste_sim(config_file: str):
     for (i, dist_values) in enumerate(p.dist):
         # noinspection PyCallingNonCallable
         dist = p.dist.dist_type(**dist_values, rng=rng)
-        chunks = int(0.6 * t_max / dist_values.get('tau', 1)) + 1
 
-        # second loop over parameter of motional model
+        # second loop over parameter of motion model
         for (j, motion_values) in enumerate(p.motion):
             # noinspection PyCallingNonCallable
             motion = p.motion.model(delta, eta, **motion_values, rng=rng)
 
-            print(f'\nStart of {dist} and {motion}')
+            print(f'\nStart of {dist}, {motion}')
 
-            start = time()
+            start = last_print = perf_counter()
 
             cc = np.zeros((len(t_mix), len(t_evo)))
             ss = np.zeros((len(t_mix), len(t_evo)))
 
             # inner loop to create trajectories
             for n in range(num_traj):
-                phase = make_trajectory(chunks, dist, motion, t_max)
+                phase = make_trajectory(dist, motion, t_max)
 
                 for (k, t_evo_k) in enumerate(t_evo):
                     dephased = phase(t_evo_k)
-                    t0= t_mix + t_evo_k
+                    t0 = t_mix + t_evo_k
                     rephased = phase(t0 + t_evo_k + 2*t_echo) + phase(t0) - 2 * phase(t0+t_echo)
                     cc[:, k] += np.cos(dephased)*np.cos(rephased)
                     ss[:, k] += np.sin(dephased)*np.sin(rephased)
 
-                print_step(n, num_traj, start)
+                last_print = print_step(n, num_traj, start, last_print)
 
             cc[:, 1:] /= num_traj
             ss[:, 1:] /= num_traj
@@ -101,11 +102,9 @@ def run_spectrum_sim(config_file: str):
     p = parse(config_file)
 
     rng, num_traj, t_max, delta, eta, num_variables = _prepare_sim(p)
-    print(num_traj)
 
     num_echos = len(p.spec.t_echo)
     reduction_factor = np.zeros((num_variables, num_echos))
-    freq = np.fft.fftshift(np.fft.fftfreq(p.spec.num_points, p.spec.dwell_time))
     t_echo = p.spec.t_echo
     t_echo_strings = list(map(str, t_echo))
 
@@ -113,23 +112,20 @@ def run_spectrum_sim(config_file: str):
     for (i, dist_values) in enumerate(p.dist):
         # noinspection PyCallingNonCallable
         dist = p.dist.dist_type(**dist_values, rng=rng)
-        print(f'\nStart of {dist}')
-
-        chunks = int(0.6 * t_max / dist.mean_tau) + 1
-
-        # second loop over parameter of motional model
+        # second loop over parameter of motion model
         for (j, motion_values) in enumerate(p.motion):
             # noinspection PyCallingNonCallable
             motion = p.motion.model(delta, eta, **motion_values, rng=rng)
-            print(f'Start of {motion}')
+            print(f'\nStart of {dist}, {motion}')
 
             timesignal = np.zeros((p.spec.num_points, num_echos))
 
-            start = time()
+            start = perf_counter()
+            last_print = start
 
             # inner loop to create trajectories
             for n in range(num_traj):
-                phase = make_trajectory(chunks, dist, motion, t_max)
+                phase = make_trajectory(dist, motion, t_max)
 
                 for (k, t_echo_k) in enumerate(t_echo):
                     # effect of de-phasing and re-phasing
@@ -139,59 +135,61 @@ def run_spectrum_sim(config_file: str):
                     timesignal[:, k] += np.cos(start_amp + phase(p.spec.t_acq + 2*t_echo_k))
                     reduction_factor[max(p.motion.num_variables, 1)*i+j, k] += np.cos(phase(2*t_echo_k) + start_amp)
 
-                print_step(n, num_traj, start)
+                # print(n+1, num_traj, start, last_print)
+                last_print = print_step(n+1, num_traj, start, last_print)
 
+            # apply line broadening
             timesignal *= p.spec.dampening[:, None]
             timesignal /= num_traj
+            timesignal[0, :] /= 2
 
             # FT to spectrum
             spec = np.fft.fftshift(np.fft.fft(timesignal, axis=0), axes=0).real
             spec -= spec[0]
+            spec *= p.spec.pulse_attn[:, None]
 
-            # plot spectra
-            fig, ax = plt.subplots()
-            lines = ax.plot(freq, spec)
-            ax.set_title(f'{dist}, {motion}')
-            ax.legend(lines, t_echo_strings)
-
-            plt.show()
+            save_spectrum_data(timesignal, spec, p, dist, motion, t_echo_strings)
 
     fig2, ax2 = plt.subplots()
-    ax2.semilogx(p.dist.variables['tau'], reduction_factor / num_traj, 'o--')
+    lines = ax2.semilogx(p.dist.variables['tau'], reduction_factor / num_traj, 'o--')
+    ax2.legend(lines, t_echo_strings)
+    plt.savefig(f'{dist.name}_{motion.name}_reduction.png')
 
     plt.show()
 
 
-def print_step(n, num_traj, start):
-    n_1 = n+1
-    if n_1 % 200 == 0 or n_1 == num_traj:
-        elapsed = time() - start
-        print(f'Step {n_1} of {num_traj}', end=' - ')
-        total = num_traj * elapsed / (n_1)
-        print(f'total: {total:.2f}s - elapsed: {elapsed:.2f}s - remaining: {total - elapsed:.2f}s')
+def make_trajectory(
+        dist: BaseDistribution,
+        motion: BaseMotion,
+        t_max: float,
+        t_passed: float = 0.,
+        init_phase: float = 0.
+):
 
-
-def make_trajectory(chunks: int, dist: BaseDistribution, motion: BaseMotion, t_max: float):
+    # set initial orientations and correlation times
     motion.start()
     dist.start()
 
-    t_passed = 0
-    t = [0]
-    phase = [0]
+    # number of jumps that are simulated at once
+    chunks = min(int(0.51 * t_max / dist.tau_jump), 100_000) + 1
+
+    t = [np.array([t_passed])]
+    phase = [np.array([init_phase])]
     while t_passed < t_max:
         # frequencies between jumps
         current_omega = motion.jump(size=chunks)
-
         # times at a particular position
         t_wait = dist.wait(size=chunks)
 
         accumulated_phase = np.cumsum(t_wait * current_omega) + phase[-1]
+        phase.append(accumulated_phase)
 
         t_wait = np.cumsum(t_wait) + t_passed
         t_passed = t_wait[-1]
-        t.extend(t_wait.tolist())
+        t.append(t_wait)
 
-        phase.extend(accumulated_phase.tolist())
+    t = np.concatenate(t)
+    phase = np.concatenate(phase)
 
     # convenient interpolation to get phase at arbitrary times
     phase_interpol = interp1d(t, phase)
@@ -200,6 +198,8 @@ def make_trajectory(chunks: int, dist: BaseDistribution, motion: BaseMotion, t_m
 
 
 def _prepare_sim(parameter: Parameter) -> tuple[Generator, int, float, float, float, int]:
+    # collect variables that are common to spectra and stimulated echo
+
     # random number generator
     rng = np.random.default_rng(parameter.sim.seed)
 
@@ -217,6 +217,56 @@ def _prepare_sim(parameter: Parameter) -> tuple[Generator, int, float, float, fl
     return rng, num_traj, t_max, delta, eta, num_variables
 
 
-def ste(x, a, f_infty, tau, beta):
-    return a*((1-f_infty) * np.exp(-(x/tau)**beta) + f_infty)
+def print_step(n: int, num_traj: int, start: float, last_print: float) -> float:
+    step_time = perf_counter()
+    dt = step_time - last_print
+    if dt > 10 or n == num_traj:
+        date = datetime.now().strftime('%Y-%m-%d %H:%M:%S')
+        print(f'{date} - step {n} of {num_traj}', end=' - ')
 
+        elapsed = step_time - start
+        total = num_traj * elapsed / n
+        print(f'expected total: {total:.2f}s - elapsed: {elapsed:.2f}s - remaining: {total - elapsed:.2f}s')
+        if dt > 10:
+            last_print = step_time
+
+    return last_print
+
+
+def make_filename(dist: BaseDistribution, motion: BaseMotion) -> str:
+    filename = f'{dist}_{motion}'
+    filename = filename.replace(' ', '_')
+    filename = filename.replace('.', 'p')
+
+    return filename
+
+
+def save_spectrum_data(
+        timesignal: np.ndarray,
+        spectrum: np.ndarray,
+        param: Parameter,
+        dist: BaseDistribution,
+        motion: BaseMotion,
+        echo_strings: list[str]
+):
+    filename = make_filename(dist, motion)
+
+    header = param.totext(sim=True, spec=True)
+    header += '\nx\t' + '\t'.join(echo_strings)
+
+    np.savetxt(filename + '_timesignal.dat', np.c_[param.spec.t_acq, timesignal], header=header)
+    np.savetxt(filename + '_spectrum.dat', np.c_[param.spec.freq, spectrum], header=header)
+
+    fig, ax = plt.subplots()
+    lines = ax.plot(param.spec.freq, spectrum)
+    ax.set_title(f'{dist}, {motion}')
+    ax.legend(lines, echo_strings)
+    plt.savefig(filename + '_spectrum.png')
+
+    fig1, ax1 = plt.subplots()
+    lines = ax1.plot(param.spec.t_acq, timesignal)
+    ax1.set_title(f'{dist}, {motion}')
+    ax1.legend(lines, echo_strings)
+    plt.savefig(filename + '_timesignal.png')
+
+    plt.show()
diff --git a/src/rwsims/spectrum.py b/src/rwsims/spectrum.py
new file mode 100644
index 0000000..e69de29
diff --git a/src/rwsims/ste.py b/src/rwsims/ste.py
new file mode 100644
index 0000000..e69de29