diff --git a/src/simulate.jl b/src/simulate.jl
index 59fdbf2..acf49d7 100644
--- a/src/simulate.jl
+++ b/src/simulate.jl
@@ -75,16 +75,16 @@ Run a simulation for the given model, simulation plan and exogenous data.
     * `model` - the [`Model`](@ref ModelBaseEcon.Model) instance to simulate.
     * `plan` - the [`Plan`](@ref) for the simulation.
     * `data` - a 2D `Array` containing the exogenous data. This includes the
-        initial and final conditions.
+  initial and final conditions.
 
 ### Options as keyword arguments
     * `fctype::`[`FinalCondition`](@ref) - set the desired final condition type
-        for the simulation. The default value is [`fcgiven`](@ref). Other possible
+  for the simulation. The default value is [`fcgiven`](@ref). Other possible
         values include [`fclevel`](@ref), [`fcslope`](@ref) and
-        [`fcnatural`](@ref).
+  [`fcnatural`](@ref).
     * `initial_guess::AbstractMatrix{Float64}` - a 2D `Array` containing the
-        initial guess for the solution. This is used to start the Newton-Raphson
-        algorithm. The default value is an empty array (`zeros(0,0)`), in which case
+  initial guess for the solution. This is used to start the Newton-Raphson
+  algorithm. The default value is an empty array (`zeros(0,0)`), in which case
         we use the exogenous data for the initial condition. You can use the steady
         state solution using [`steadystatearray`](@ref).
     * `deviation::Bool` - set to `true` if the `data` is given in deviations from
@@ -97,10 +97,10 @@ Run a simulation for the given model, simulation plan and exogenous data.
     * `verbose::Bool` - control whether or not to print progress information.
         Default value is taken from `model.options`.
     * `tol::Float64` - set the desired accuracy. Default value is taken from
-        `model.options`.
+  `model.options`.
     * `maxiter::Int` - algorithm fails if the desired accuracy is not reached
         within this maximum number of iterations. Default value is taken from
-        `model.options`.
+  `model.options`.
 The following options are specific to the `:stackedtime` solver
     * `sim_solver` - specify the non-linear solver to use. Available options are 
       - `:sim_nr` : (default) Newton-Raphson, with possible damping, see below.
@@ -111,7 +111,7 @@ The following options are specific to the `:stackedtime` solver
       will do this at each iteration. Default is `false`. (Superseded by the
       `damping` option described below)
     * `damping` - Specifies the style of damping that can be applied to the
-      Newton non-linear solver. Available options are:
+  Newton non-linear solver. Available options are:
       - if not given the default behaviour is no damping, i.e. the damping
         coefficient is set to 1.0 in each iteration.
       - number: the damping coefficient will be set to the given number (rather than 1)
@@ -122,13 +122,11 @@ The following options are specific to the `:stackedtime` solver
       - `:linesearch` or `:armijo` : same as setting `linesearch=true`. The
         Armijo rule is taken from "C.T.Kelly, Iterative Methods for Linear and
         Nonlinear Equations, ch.8.1, p.137"
-      - `(:armijo, :sigma => 0.5, :alpha => 1e-4)` - override the default
-        parameters of the Armijo rule.
-      - `:br81` : (experimental) implements the damping algorithm in "Bank, R.E.,
-        Rose, D.J. Global approximate Newton methods. Numer. Math. 37, 279–295
-        (1981)."
-      - `(:br81, :rateK => 10, :delta => 0.1)` : override the default parameters
-        of the Bank & Rose (1981) algorithm.
+      - `(:armijo, :sigma => 0.5, :alpha => 1e-4, :lambda_min => 1e-5, :lambda_max => 1.0, :lambda_growth => 1.05)` - 
+      extends the Armijo rule with additional controls for minimum and maximum damping factors and a lambda growth parameter.
+      - `:br81` - (experimental) implements the damping algorithm from "Bank, R.E., Rose, D.J. Global approximate Newton methods. Numer. Math. 37, 279–295 (1981)."
+      - `(:br81, :rateK => 10, :delta => 0.1, :lambda_min => 1e-5, :lambda_max => 1.0, :lambda_growth => 1.05)`
+      - extends `:br81` with additional controls for minimum and maximum damping factors and a lambda growth parameter.
 
 """
 function simulate end
diff --git a/src/stackedtime/sim_nr.jl b/src/stackedtime/sim_nr.jl
index 51c7068..6c61738 100644
--- a/src/stackedtime/sim_nr.jl
+++ b/src/stackedtime/sim_nr.jl
@@ -24,21 +24,21 @@ Solve the simulation problem using a Newton iteration with damping.
     - `damping_schedule(vector)` returns `λ=vector[it]` on iteration `it`. If
       the vector is shorter than the number of iterations, it keeps returning
       `array[end]`.
-    - `damping_amijo(α=1e-4, σ=0.5)` implements a standard linesearch algorithm
+    - `damping_amijo(sigma = 0.5, alpha = 1e-4, lambda_min = 1e-5, lambda_max = 1.0, lambda_growth = 1.05)` implements a standard linesearch algorithm
       based on the Armijo rule
-    - `damping_bank_rose(delta=0.1, rateK=10.0)` implements a the damping
-      algorithm of Bank and Rose 1980
-
+    - `damping_br81(delta = 0.1, lambda_min = 1e-5, lambda_max = 1.0, lambda_growth = 1.05)` implements a the damping
+      algorithm of Bank and Rose (1981)
+    
 ##### Conventions for custom damping function.
 The `damping` callback function is expected to have the following signature:
-
+    
     function custom_damping(k::Int, λ::Float64, nR::Float64, R::AbstractVector{Float64},
         J::Union{Nothing,Factorization,AbstractMatrix{Float64}}=nothing,
         Δx::Union{Nothing,AbstractVector{Float64}}=nothing
     )::Tuple{Bool, Float64}
         # <your code goes here>
     end
-
+    
 The first call will be with `k=0`, before the solver enters the Newton
 iterations loop. This should allow any initialization and defaults to be setup.
 In this call, the values of `R` and `nR` will equal the residual and its norm at
@@ -49,7 +49,7 @@ Each subsequent call will be with `k` between 1 and `maxiter` (possibly multiple
 calls with the same `k`) will have the current `λ` (which equals the one returned by the
 previous call), the current `R` (and its Inf-norm `nR`), the Jacobian `J` and
 the Newton direction `Δx`.
-
+    
 The damping function must return a tuple `(accept, λ)`. The same Newton
 iteration `k` will continue until the damping function returns `accept=true`,
 after which will begin the next Newton iteration (`k=k+1``).
@@ -69,7 +69,7 @@ to accept this step, by returning `(true, λ)`, or reject it and propose a new 
 to try, by returning `(false, new_λ)`. Don't return `(false, λ)` because this
 will make it an infinite loop. Good luck!
 
-"""
+    """
 function sim_nr!(x::AbstractArray{Float64}, sd::StackedTimeSolverData,
     maxiter::Int64, tol::Float64, verbose::Bool, damping::Function
 )
@@ -141,44 +141,63 @@ function damping_schedule(lambda::AbstractVector{<:Real}; verbose::Bool=false)
 end
 
 # the Armijo rule: C.T.Kelly, Iterative Methods for Linear and Nonlinear Equations, ch.8.1, p.137
-function damping_armijo(; alpha::Real=1e-4, sigma::Real=0.5, lambda_min::Real=0.00001, verbose::Bool=false)
+function damping_armijo(; alpha::Real=1e-4, sigma::Real=0.5, lambda_min::Real=1e-5, lambda_max::Real=1.0, lambda_growth::Real=1.1, verbose::Bool=false)
     α = convert(Float64, alpha)
     σ = convert(Float64, sigma)
     λ_min = convert(Float64, lambda_min)
+    λ_max = convert(Float64, lambda_max)
+    λ_growth = convert(Float64, lambda_growth)
     nF2_it = 0  # iteration number at which nF2 is valid
     nF2 = NaN   # the norm of the residual at the beginning of iteration nF2_it
     return function (it::Int, λ::Float64, nF::Float64, F::AbstractVector{Float64},
         ::Union{Nothing,Factorization,AbstractMatrix{Float64}}=nothing,
         ::Union{Nothing,AbstractVector{Float64}}=nothing
     )
-        # @printf "    it=%d, λ=%g, nF=%g\n" it λ nF
-        it < 1 && return true, 1.0
+        it < 1 && return true, min(1.0, λ_max)  
+
         if nF2_it != it
-            # first time we're called this iteration 
-            nF2 = norm(F, 2)  # store the residual 
+            # First call in this iteration: Store the residual norm
+            nF2 = norm(F, 2)
             nF2_it = it
-            return false, 1.0   # try λ=1.0, a full Newton step, first
+            return false, min(1.0, λ_max)  
         end
+
         if λ < λ_min
-            # λ too small
-            verbose && @warn "Linesearch failed."
+            verbose && @warn "Linesearch failed: λ fell below λ_min."
             return true, λ
         end
+
         if norm(F, 2) < (1.0 - α * λ) * nF2
-            # Armijo test pass => accept the given λ
-            return true, λ
+            # Armijo test passed => accept the given λ
+            new_λ = min(λ * λ_growth, λ_max)  # Gradually increase λ but cap at λ_max
+            
+            if abs(norm(F, 2) - nF2) < 1e-12  # Convergence check to break loops
+                verbose && @info "Solver converged: residual change too small."
+                return true, new_λ
+            end
+
+            return true, new_λ
         else
-            # reject and try a smaller λ
-            return false, σ * λ
+            # Reject and try a smaller λ
+            new_λ = max(σ * λ, λ_min)
+            
+            if λ == new_λ  # Prevent infinite shrinking loops
+                verbose && @warn "Stuck in shrinking loop, forcing exit."
+                return true, λ
+            end
+
+            return false, new_λ
         end
     end
 end
 
 # Bank, R.E., Rose, D.J. Global approximate Newton methods. Numer. Math. 37, 279–295 (1981). 
 # https://doi.org/10.1007/BF01398257
-function damping_br81(; delta::Real=0.1, rateK::Real=10.0, lambda_min::Real=1e-5, verbose::Bool=false)
+function damping_br81(; delta::Real=0.1, rateK::Real=10.0, lambda_min::Real=1e-5, lambda_max::Real=1.0, lambda_growth::Real=1.05, verbose::Bool=false)
     δ = convert(Float64, delta)
     λ_min = convert(Float64, lambda_min)
+    λ_max = convert(Float64, lambda_max)
+    λ_growth = convert(Float64, lambda_growth)
     bigK = 0.0  # Initialize with 0.0 (effectively the full Newton step)
     nF2_it = 0  # iteration number at which nF2 is valid
     nF2 = NaN   # the norm of the residual at the beginning of iteration nF2_it
@@ -187,33 +206,37 @@ function damping_br81(; delta::Real=0.1, rateK::Real=10.0, lambda_min::Real=1e-5
         ::Union{Nothing,Factorization,AbstractMatrix{Float64}}=nothing,
         ::Union{Nothing,AbstractVector{Float64}}=nothing
     )
-        # @printf "    it=%d, λ=%g, nF=%g\n" it λ nF
-        it < 1 && (bigK = 0.0; return true, 1.0)
+        # Initialization step
+        it < 1 && (bigK = 0.0; return true, λ_max)
+        
         if nF2_it != it
-            # first time we're called this iteration 
+            # First time we're called in this iteration
             nF2 = norm(F, 2)  # store the residual 
             nF2_it = it
             return false, calc_λ()
         end
+        
         if (1 - δ * λ) * nF2 < norm(F, 2)
-            # test failed => reject and try smaller λ
+            # If test failed, decrease step size
             if bigK == 0.0
                 bigK = 1.0
             else
-                bigK = rateK * bigK
+                bigK *= rateK  # Increase `bigK` slower to prevent excessive reductions in λ
             end
             λ = calc_λ()
             if λ > λ_min
                 return false, λ
             else
-                # λ too small
                 verbose && @warn "Linesearch failed."
                 return true, λ_min
             end
         else
-            # lower bigK for next iteration ...
-            bigK = bigK / rateK
-            # ... and accept given λ 
+            # Lower `bigK` more aggressively when convergence is happening
+            bigK /= sqrt(rateK)
+
+            # If λ is near the lower bound for many steps, slowly increase it
+            λ = min(λ * λ_growth, λ_max)
+
             return true, λ
         end
     end