#include <bits/stdc++.h>
using namespace std;
#define int long long int
#define double long double
#define print(a) for(auto x : a) cout << x << " "; cout << endl
const int M = 1000000007;
const int N = 3e5+9;
const int INF = 2e9+1;
const int LINF = 2000000000000000001;
inline int power(int a, int b, int mod=M) {
int x = 1;
a %= mod;
while (b) {
if (b & 1) x = (x * a) % mod;
a = (a * a) % mod;
b >>= 1;
}
return x;
}
//_ ***************************** START Below *******************************
string a;
vector<vector<int>> qr;
vector<int> consistency(int n, int q){
vector<vector<int>> mp(n+1, vector<int>(26, 0));
for(int i=0; i<n; i++){
mp[i+1] = mp[i];
mp[i+1][a[i] - 'a']++;
}
vector<int> ans;
for(auto& qq : qr){
int L = qq[0];
int R = qq[1];
int val = 0;
for(int j=0; j<26; j++){
int ct = mp[R][j] - mp[L-1][j];
val += (ct * (ct+1))/2;
}
ans.push_back(val);
}
return ans;
}
vector<int> practice(int n, int q){
}
void solve() {
int n, q;
cin>> n >> q;
cin >> a;
qr.resize(q);
for(int i=0; i<q; i++) {
int x, y;
cin >> x >> y;
qr[i] = {x,y};
}
auto ans = consistency(n, q);
for(auto& t : ans) cout << t << " "; cout << endl;
}
int32_t main() {
ios_base::sync_with_stdio(0); cin.tie(0); cout.tie(0);
int t = 1;
// cin >> t;
while (t--) {
solve();
}
return 0;
}
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