#include <bits/stdc++.h>
using namespace std;
#define int long long int
#define double long double
inline int power(int a, int b) {
int x = 1;
while (b) {
if (b & 1) x *= a;
a *= a;
b >>= 1;
}
return x;
}
const int M = 1000000007;
const int N = 3e5+9;
const int INF = 2e9+1;
const int LINF = 2000000000000000001;
//_ ***************************** START Below *******************************
// dddeeeeeeeeeeepp deep
void consistency(string s, string t) {
int n = s.size();
int m = t.size();
vector<int> f(26, 0), g(26, 0);
for(int i=0; i<n; i++){
f[s[i]-'a']++;
}
for(int i=0; i<m; i++){
g[t[i]-'a']++;
}
int ans = INF;
for(int i=0; i<26; i++){
if(g[i] == 0) continue;
//* if any s freq < t freq then t can't fit in s => return 0
if(f[i] < g[i]){
cout << 0 << endl;
return;
}
f[i] = f[i]/g[i];
ans = min(ans, f[i]);
}
cout << ans << endl;
}
void solve() {
string s, t;
cin >> s >> t;
consistency(s, t) ;
}
int32_t main() {
ios_base::sync_with_stdio(0); cin.tie(0); cout.tie(0);
int t = 1;
while (t--) {
solve();
}
return 0;
}
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